#### Abstract

The mechanism responsible for the prompt emission of gamma-ray bursts (GRBs) is still a debated issue. The prompt phase-related GRB correlations can allow discriminating among the most plausible theoretical models explaining this emission. We present an overview of the observational two-parameter correlations, their physical interpretations, and their use as redshift estimators and possibly as cosmological tools. The nowadays challenge is to make GRBs, the farthest stellar-scaled objects observed (up to redshift ), standard candles through well established and robust correlations. However, GRBs spanning several orders of magnitude in their energetics are far from being standard candles. We describe the advances in the prompt correlation research in the past decades, with particular focus paid to the discoveries in the last 20 years.

#### 1. Introduction

Gamma-ray bursts (GRBs) are highly energetic events with the total isotropic energy released of the order of (for recent reviews, see [1–6]). GRBs were discovered by military satellites* Vela* in late 1960s and were recognized early to be of extrasolar origin [7]. A bimodal structure (reported first by Mazets et al. [8]) in the duration distribution of GRBs detected by the Burst and Transient Source Experiment (BATSE) onboard the* Compton Gamma-Ray Observatory* (CGRO) [9], based on which GRBs are nowadays commonly classified into short (with durations , SGRBs) and long (with , LGRBs), was found [10]. BATSE observations allowed also confirming the hypothesis of Klebesadel et al. [7] that GRBs are of extragalactic origin due to isotropic angular distribution in the sky combined with the fact that they exhibited an intensity distribution that deviated strongly from the power law [9, 11–14]. This was later corroborated by establishing the first redshift measurement, taken for GRB970508, which with was placed at a cosmological distance of at least 2.9 Gpc [15]. Despite initial isotropy, SGRBs were shown to be distributed anisotropically on the sky, while LGRBs are distributed isotropically [16–23]. Cosmological consequences of the anisotropic celestial distribution of SGRBs were discussed lately by Mészáros et al. [24] and Mészáros and Rees [6]. Finally, the progenitors of LGRBs are associated with supernovae (SNe) [25–29] related to collapse of massive stars. Progenitors of SGRBs are thought to be neutron star–black hole (NS–BH) or NS–NS mergers [12, 30–32], and no connection between SGRBs and SNe has been proven [33].

While the recent first direct detection of gravitational waves (GW), termed GW150914, by the Laser Interferometer Gravitational Wave Observatory (LIGO) [34], interpreted as a merger of two stellar-mass BHs with masses and , is by itself a discovery of prime importance, it becomes especially interesting in light of the finding of Connaughton et al. [35] who reported a weak transient source lasting 1 s and detected by* Fermi*/GBM [36] only 0.4 s after the GW150914, termed GW150914-GBM. Its false alarm probability is estimated to be 0.0022. The fluence in the energy band 1 keV–10 MeV is computed to be . While these GW and GRB events are consistent in direction, its connection is tentative due to relatively large uncertainties in their localization. This association is unexpected as SGRBs have been thought to originate from NS–NS or NS–BH mergers. Moreover, neither* INTEGRAL* [37] nor* Swift* [38] detected any signals that could be ascribed to a GRB. Even if it turns out that it is only a chance coincidence [39], it has already triggered scenarios explaining how a BH–BH merger can become a GRB; for example, the nascent BH could generate a GRB via accretion of a mass *≃* 10^{−5}* M*_{⊙} [40], indicating its location in a dense medium (see also [41]), or two high-mass, low-metallicity stars could undergo an SN explosion, and the matter ejected from the last exploding star can form—after some time—an accretion disk producing an SGRB [42]. Also the possible detection of an afterglow that can be visible many months after the event [43] could shed light on the nature of the GW and SGRB association.

From a phenomenological point of view, a GRB is composed of the prompt emission, which consists of high-energy photons such as -rays and hard X-rays, and the afterglow emission, that is, a long lasting multiwavelength emission (X-ray, optical, and sometimes also radio), which follows the prompt phase. The first afterglow observation (for GRB970228) was due to the* BeppoSAX* satellite [44, 45]. Another class, besides SGRBs and LGRBs, that is, intermediate in duration, was proposed to be present in univariate duration distributions [46–51], as well as in higher dimensional parameter spaces [51–56]. On the other hand, this elusive intermediate class might be a statistical feature that can be explained by modeling the duration distribution with skewed distributions, instead of the commonly applied standard Gaussians [57–61]. Additionally, GRB classification was shown to be detector-dependent [1, 62, 63]. Moreover, a subclass classification of LGRBs was proposed [64], and Norris and Bonnell [65] discovered the existence of an intermediate class or SGRBs with extended emission, that show mixed properties between SGRBs and LGRBs. GRBs with very long durations (ultralong GRBs, with ) are statistically different than regular (i.e., with ) LGRBs [66] and hence might form a different class (see also [67–70]). Another relevant classification appears related to the spectral features distinguishing normal GRBs from X-ray flashes (XRFs). The XRFs [71, 72] are extragalactic transient X-ray sources with spatial distribution and spectral and temporal characteristics similar to LGRBs. The remarkable property that distinguishes XRFs from GRBs is that their prompt emission spectrum peaks at energies which are observed to be typically an order of magnitude lower than the observed peak energies of GRBs. XRFs are empirically defined by a greater fluence (time-integrated flux) in the X-ray band () than in the -ray band (). This classification is also relevant for the investigation of GRB correlations since some of them become stronger or weaker by introducing different GRB categories. Grupe et al. [73], using 754* Swift* GRBs, performed an exhaustive analysis of several correlations as well as the GRB redshift distribution, discovering that the bright bursts are more common in the high- (i.e., than in the local universe.

This classification has further enhanced the knowledge of the progenitor system from which GRBs originate. It was soon after their discovery that LGRBs were thought to originate from distant star-forming galaxies. Since then, LGRBs have been firmly associated with powerful core-collapse SNe and the association seems solid. Nevertheless, there have been puzzling cases of LGRBs that were not associated with bright SNe [74, 75]. This implies that it is possible to observe GRBs without an associated bright SNe or there are other progenitors for LGRBs than core-collapse of massive stars. Another relevant uncertainty concerning the progenitor systems for LGRBs is the role of metallicity . In the collapsar model [27], LGRBs are only formed by massive stars with below . However, several GRBs have been located in very metal-rich systems [76] and it is an important goal to understand whether there are other ways to form LGRBs than through the collapsar scenario [77]. One of the models used to explain the GRB phenomenon is the “fireball” model [78–80] in which a compact central engine (either the collapsed core of a massive star or the merger product of an NS–NS binary) launches a highly relativistic, jetted electron-positron-baryon plasma. Interactions of blobs within the jet are believed to produce the prompt emission. Instead, the interaction of the jet with the ambient material causes the afterglow phase. However, problems in explaining the light curves within this model have been shown by Willingale et al. [81]. Specifically, for *≃*50% of GRBs, the observed afterglows are in agreement with the model, but for the rest the temporal and spectral indices do not conform and suggest a continued late energy injection. Melandri et al. [82] performed a multiwavelength analysis and found that the forward shock (FS) model does not explain almost 50% of the examined GRBs, even after taking into account energy injection. Rykoff et al. [83] showed that the fireball model does not model correctly early afterglows. Reference [84] analysed the prompt and afterglow light curves and pointed out that some GRBs required energy injection to explain the outflows. The crisis of the standard fireball models appeared when* Swift* [85] observations revealed a more complex behaviour of the light curves than observed in the past [86–88] and pointed out that GRBs often follow “canonical” light curves [89]. Therefore, the discovery of correlations among relevant physical parameters in the prompt phase is very important in this context in order to use them as possible model discriminators. In fact, many theoretical models have been presented in the literature in order to explain the wide variety of observations, but each model has some advantages as well as drawbacks, and the use of the phenomenological correlations can boost the understanding of the mechanism responsible for the prompt emission. Moreover, given the much larger (compared to SNe) redshift range over which GRBs can be observed, it is tempting to include them as cosmological probes, extending the redshift range by almost an order of magnitude further than the available SNe Ia. GRBs are observed up to redshift [90], much more distant than SNe Ia, observed up to [91], and therefore they can help to understand the nature of dark energy and determine the evolution of its equation of state at very high . However, contrary to SNe Ia, which originate from white dwarves reaching the Chandrasekhar limit and always releasing the same amount of energy, GRBs cannot yet be considered standard candles with their (isotropic-equivalent) energies spanning 8 orders of magnitude (see also [92] and references therein). Therefore, finding universal relations among observable properties can help to standardize their energetics and/or luminosities. They can serve as a tracer of the history of the cosmic star formation rate [93–97] and provide invaluable information on the physics in the intergalactic medium [98–100]. This is the reason why the study of GRB correlations is so relevant for understanding the GRB emission mechanism, for finding a good distance indicator, and for exploring the high-redshift universe [101].

This paper is organized in the following manner. In Section 2, we explain the nomenclature and definitions adopted in this work, and in Section 3 we analyse the correlations between various prompt parameters. We summarize in Section 4.

#### 2. Notations and Nomenclature

For clarity we report a summary of the nomenclature adopted in the review. , , , , and indicate the luminosity, the energy flux, the energy, the fluence, and the timescale, respectively, which can be measured in several wavelengths. More specifically,(i) is the time interval in which 90% of the GRB’s fluence is accumulated, starting from the time at which 5% of the total fluence was detected [10];(ii) is defined, similar to , as the time interval from 25% to 75% of the total detected fluence;(iii) is the time spanned by the brightest 45% of the total counts detected above background [102];(iv) is the time at which the pulse (i.e., a sharp rise and a slower, smooth decay [103–106]) in the prompt light curve peaks (see Figure 1);(v) is the time of a power law break in the afterglow light curve [107, 108], that is, the time when the afterglow brightness has a power law decline that suddenly steepens due to the slowing down of the jet until the relativistic beaming angle roughly equals the jet-opening angle [109];(vi) and are the difference of arrival times to the observer of the high-energy photons and low energy photons defined between and energy band and the shortest time over which the light curve increases by of the peak flux of the pulse;(vii) is the end time prompt phase at which the exponential decay switches to a power law, which is usually followed by a shallow decay called the plateau phase, and is the time at the end of this plateau phase [81];(viii) is the pulse width since the burst trigger at the time of the ejecta;(ix), , , and are the peak energy, that is, the energy at the peak of the spectrum [110], the total isotropic energy emitted during the whole burst (e.g., [111]), the total energy corrected for the beaming factor [the latter two are connected via ], and the isotropic energy emitted in the prompt phase, respectively;(x), are the peak and the total fluxes, respectively [112];(xi), , and are the luminosities respective to , (specified in the X-ray band), and ;(xii) is the observed luminosity, and specifically and are the peak luminosity (i.e., the luminosity at the pulse peak, [113]) and the total isotropic luminosity, both in a given energy band. More precisely, is defined as follows:with the luminosity distance given bywhere and are the matter and dark energy density parameters, is the present-day Hubble constant, and is the redshift. Similarly, is given by(xiii), , indicate the prompt fluence in the whole gamma band (i.e., from a few hundred keV to a few MeV), the observed fluence in the range , and the total fluence in the energy band;(xiv) is the variability of the GRB’s light curve. It is computed by taking the difference between the observed light curve and its smoothed version, squaring this difference, summing these squared differences over time intervals, and appropriately normalizing the resulting sum [102]. Different smoothing filters may be applied (see also [114] for a different approach). denotes the variability for a certain fraction of the smoothing timescale in the light curve.

Most of the quantities described above are given in the observer frame, except for , , , and , which are already defined in the rest frame. With the upper index “” we explicitly denote the observables in the GRB rest frame. The rest frame times are the observed times divided by the cosmic time expansion; for example the rest frame time in the prompt phase is denoted by . The energetics are transformed differently, for example, .

The Band function [115] is a commonly applied phenomenological spectral profile, such thatwhere is the normalization. Here, and are the low- and high-energy indices of the Band function, respectively. is in units of photons cm^{−2} s^{−1} keV^{−1}. For the cases and , can be derived as , which corresponds to the energy at the maximum flux in the spectra [115, 116].

The Pearson correlation coefficient [117, 118] is denoted by , the Spearman correlation coefficient [119] is denoted by , and the value (a probability that a correlation is drawn by chance) is denoted by .

Finally, we mostly deal with correlations of the form . However, when the intercept is neglected in the text, but its value is nonnegligible (or not known due to lacking in the original paper), we use the notation to emphasize the slope.

#### 3. The Prompt Correlations

Several physical relations between relevant quantities in GRBs were found since the 1990s. In each paragraph below, we follow the discovery of the correlation with the definition of the quantities, the discussions presented in literature, and their physical interpretation.

##### 3.1. The Correlation

###### 3.1.1. Literature Overview

Liang and Kargatis [120], using 34 bright GRBs detected by BATSE, found that depends linearly on the previous flux emitted by the pulse, that is, that the rate of change of is proportional to the instantaneous luminosity. Quantitativelywhere is a normalization constant expressing the luminosity for each pulse within a burst, and was calculated from the observed flux via (1).

The correlation was introduced for the first time by Norris et al. [113] who examined a sample of 174 GRBs detected by BATSE, among which 6 GRBs had an established redshift and those were used to find an anticorrelation between and in the form of the following (see Figure 2(a)):with , in units of , computed in the range, and is measured in seconds. A remarkably consistent relation was found by Schaefer et al. [121], who used a sample of 112 BATSE GRBs and reported thatbeing in perfect agreement with the result of Norris et al. [113]. Here, is in units of and in seconds. This relation has been confirmed by several studies (e.g., [122–124]).

**(a)**

**(b)**

Schaefer [125] showed that the relation is a consequence of the Liang and Kargatis [120] empirical relation from (5), and he derived this dependence to be of the form . This correlation was useful in the investigation of Kocevski and Liang [126], who used a sample of 19 BATSE GRBs and the relation from [121] to infer their pseudoredshifts. Their approach was to vary the guessed until it allowed matching the luminosity distance measured with the GRB’s energy flux and that can be calculated from the guessed redshift within a flat CDM model, until the agreement among the two converged to within . Next, the rate of decay, as in [120], was measured. Finally, Kocevski and Liang [126] showed that the is directly related to the GRB’s spectral evolution. However, Hakkila et al. [127] found a different slope, and argued that the relation is a pulse rather than a burst property; that is, each pulse is characterized by its own , distinct for various pulses within a GRB.

Tsutsui et al. [128], using pseudoredshifts estimated via the Yonetoku relation (see Section 3.6.2) for 565 BATSE GRBs, found that the relation has a of only (see Figure 2(b)). However, assuming that the luminosity is a function of both the redshift and the lag, a new redshift-dependent relation was found as

with in units of , in seconds, and . Although the spectral lag is computed from two channels of BATSE, this new relation suggests that a future lag-luminosity relation defined within the* Swift* data should also depend on the redshift.

Afterwards, Sultana et al. [129] presented a relation between the - and -corrected for the* Swift* energy bands and , and , for a subset of 12* Swift* long GRBs. The -correction takes into account the time dilatation effect by multiplying the observed lag by to translate it into the rest frame. The -correction takes into account a similar effect caused by energy bands being different in the observer and rest frames via multiplication by [130]. The net corrected is thence . In addition, Sultana et al. [129] demonstrated that this correlation in the prompt phase can be extrapolated into the relation [131–134]. Sultana et al. [129] found the following (Note that Sultana et al. [129] used to denote the peak isotropic luminosity.):with in ms, in seconds, and in . The correlation coefficient is significant for these two relations ( for the and for the relations) and has surprisingly similar best-fit power law indices ( and , resp.). Although and represent different GRB time variables, it appears distinctly that the relation extrapolates into for timescales . A discussion and comparison of this extrapolation with the relation are extensively presented in [135].

Ukwatta et al. [136] confirmed that there is a correlation between and the - and -corrected among 31 GRBs observed by* Swift*, with , and the slope equal to , hence confirming the relation, although with a large scatter. This was followed by another confirmation of this correlation [137] with the use of 43* Swift* GRBs with known redshift, which yielded , , and a slope of , being consistent with the previous results.

Finally, Margutti et al. [138] established that the X-ray flares obey the same relation (in the rest frame energy band ) as GRBs and proposed that their underlying mechanism is similar.

###### 3.1.2. Physical Interpretation of the Relation

The physical assumption on which the work by Norris et al. [113] was based is that the initial mechanism for the energy formation affects the development of the pulse much more than dissipation. From the study of several pulses in bright, long BATSE GRBs, it was claimed that, for pulses with precisely defined shape, the rise-to-decay ratio is ≤1. In addition, when the ratio diminishes, pulses show a tendency to be broader and weaker.

Salmonson [122] proposed that the relation arises from an entirely kinematic effect. In this scenario, an emitting region with constant (among the bursts) luminosity is the source of the GRB’s radiation. He also claimed that variations in the line-of-sight velocity should affect the observed luminosity proportionally to the Lorentz factor of the jet’s expansion, (where is the relative velocity between the inertial reference frames and is the speed of light), while the apparent is proportional to . The variations in the velocity among the lines of sight is a result of the jet’s expansion velocity combined with the cosmological expansion. The differences of luminosity and lag between different bursts are due to the different velocities of the individual emitting regions. In this case, the luminosity is expected to be proportional to , which is consistent with the observed relation. This explanation, however, requires the comoving luminosity to be nearly constant among the bursts, which is a very strong condition to be fulfilled. Moreover, this scenario has several other problems (as pointed out by Schaefer [125]):(1)It requires the Lorentz factor and luminosity to have the same range of variation. However, the observed span more than three orders of magnitude (e.g., [121]), while the Lorentz factors span less than one order of magnitude (i.e., a factor of 5) [139].(2)It follows that the observed luminosity should be linearly dependent on the jet’s Lorentz factor, yet this claim is not justified. In fact, a number of corrections are to be taken into account, leading to a significantly nonlinear dependence. The forward motion of the jet introduces by itself an additional quadratic dependence [140].

Ioka and Nakamura [141] proposed another interpretation for the correlation. From their analysis, a model in which the peak luminosity depends on the viewing angle is elaborated: the viewing angle is the off-axis angular position from which the observer examines the emission. Indeed, it is found that a high-luminosity peak in GRBs with brief spectral lag is due to an emitted jet with a smaller viewing angle than a fainter peak with extended lag. It is also claimed that the viewing angle can have implications on other correlations, such as the luminosity-variability relation presented in Section 3.2. As an additional result from this study, it was pointed out that XRFs can be seen as GRBs detected from large angles with high spectral lag and small variability.

On the other hand, regarding the jet angle distributions, Liang et al. [142] found an anticorrelation between the jet-opening angle and the isotropic kinetic energy among 179 X-ray GRB light curves and the afterglow data of 57 GRBs. Assuming that the GRB rate follows the star formation rate, and, after a careful consideration of selection effects, Lü et al. [143] found in a sample of 77 GRBs an anticorrelation between the jet-opening angle and the redshift in the following form:with and . Using a mock sample and bootstrap technique, they showed that the observed relation is most likely due to instrumental selection effects. Moreover, they argued that while other types of relation, for example, [144] or the redshift dependence of the shallow decay in X-ray afterglows by Stratta et al. [145], might have connections with the jet geometry, they are also likely to stem from observational biases or sample selection effects. Also, Ryan et al. [146] investigated the jet-opening angle properties using a sample of 226* Swift*/XRT GRBs with known redshift. They found that most of the observed afterglows were observed off-axis; hence the expected behaviour of the afterglow light curves can be significantly affected by the viewing angle.

Zhang et al. [33] argued, on the basis of the kinematic model, that the origin of the relation is due to a more intrinsic relation (see Section 3.2). They also gave an interpretation of the latter relation within the internal shock model (see Section 3.2.2). Recently, Uhm and Zhang [147] constructed a model based on the synchrotron radiation mechanism that explains the physical origin of the spectral lags and is consistent with observations.

Another explanation for the origin of the relation, given by Sultana et al. [129], involves only kinematic effects. In this case, and depend on the quantity:depicting the Doppler factor of a jet at a viewing angle and with velocity at redshift . In this study there is no reference to the masses and forces involved and, as a consequence of the Doppler effect, the factor associates the GRB rest frame timescale with the observed time in the following way:Therefore, considering a decay timescale in the GRB rest frame, (12) in the observer frame will give . Furthermore, taking into account a spectrum given by , the peak luminosity (as already pointed out by Salmonson [122]) can be computed aswith . In such a way, (12) and (13) allow retrieving the observed relation. Finally, the analogous correlation coefficients and best-fit slopes of the and correlations obtained by Sultana et al. [129] seem to hint toward a similar origin for these two relations.

##### 3.2. The Correlation

The first correlation between and was discovered by Fenimore and Ramirez-Ruiz [148] and was given as

with measured in . Here, the luminosity is per steradian in a specified (rest frame) energy bandpass , averaged over . First, seven BATSE GRBs with a measured redshift were used to calibrate the relation. Next, the obtained relationship was applied to 220 bright BATSE GRBs in order to obtain the luminosities and distances and to infer that the GRB formation rate scales as . Finally, the authors emphasized the need of confirmation of the proposed relation.

###### 3.2.1. Literature Overview

Reichart et al. [102] used a total of 20 GRBs observed by* CGRO*/BATSE (13 bursts), the* KONUS*/Wind (5 bursts), the* Ulysses*/GRB (1 burst), and the* NEAR*/XGRS (1 burst), findingwith and (see Figure 3(a)); was computed in the observer-frame energy band, which corresponds roughly to the range in the rest frame for , typical for GRBs in the sample examined. The distribution of the sample’s bursts in the plane appears to be well modeled by the following parameterization:where is the intercept of the line, is its slope, and and are the median values of and for the bursts in the sample for which spectroscopic redshifts, peak fluxes, and 64 ms or better resolution light curves are available.

**(a)**

**(b)**

**(c)**

Later, Guidorzi et al. [149] updated the sample to 32 GRBs detected by different satellites, that is,* BeppoSAX*,* CGRO*/BATSE,* HETE-2*, and* KONUS* (see Figure 3(b)). The existence of a correlation was confirmed, but they found a dramatically different relationship with respect to the original one:

with and , and in units of .

However, Reichart and Nysewander [150] using the same sample claimed that this result was the outcome of an improper statistical methodology and confirmed the previous work of Reichart et al. [102]. Indeed, they showed that the difference among their results and the ones from Guidorzi et al. [149] was due to the fact that the variance of the sample in the fit in [149] was not taken into account. They used an updated data set, finding that the fit was well described by the slope , with a sample variance .

Subsequently, Guidorzi et al. [151], using a sample of 551 BATSE GRBs with pseudoredshifts derived using the relation [152], tested the correlation (see Figure 3(c)). They also calculated the slope of the correlation of the samples using the methods implemented by Reichart et al. [102] and D'Agostini [153]. The former method provided a value of the slope in the correlation consistent with respect to the previous works:Instead, the slope for this sample using the latter method is much lower than the value in [102]:The latter slope is consistent with the results obtained by Guidorzi et al. [149], but inconsistent with the results derived by Reichart and Nysewander [150].

Afterwards, Rizzuto et al. [154] tested this correlation with a sample of 36 LGRBs detected by* Swift* in the energy range and known redshifts. The sample consisted of bright GRBs with within energy range. In their study, they adopted two definitions of variability, presented by Reichart et al. [102], called , and by Li and Paczyński [114], hereafter . and differ from each other with a different smoothing filter which, in the second case, selects only high-frequency variability. Finally, Rizzuto et al. [154] confirmed the correlation and its intrinsic dispersion around the best-fitting power law given bywith and , andwith , , and . Six low-luminosity GRBs (i.e., GRB050223, GRB050416A, GRB050803, GRB051016B, GRB060614, and GRB060729), out of a total of 36 in the sample, are outliers of the correlation, showing values of higher than expected. Thus, the correlation is not valid for low-luminosity GRBs.

As is visible from this discussion, the scatter in this relation is not negligible, thus making it less reliable than the previously discussed ones. However, investigating the physical explanation of this correlation is worth being depicted for further developments.

###### 3.2.2. Physical Interpretation of the Relation

We here briefly describe the internal and external shock model [80, 155], in which the GRB is caused by emission from a relativistic, expanding baryonic shell with a Lorentz bulk factor . Let there be a spherical section with an opening angle . In general, can be greater than , but the observer can detect radiation coming only from the angular region with size . An external shock is formed when the expanding shell collides with the external medium. In general, there might be more than one shell, and the internal shock takes place when a faster shell reaches a slower one. In both cases one distinguishes an FS, when the shock propagates into the external shell or the external medium, and a reverse shock (RS), when it propagates into the inner shell.

Fenimore and Ramirez-Ruiz [148] pointed out that the underlying cause of the relation is unclear. In the context of the internal shock model, larger initial factors tend to produce more efficient collisions. After changing some quantities such as the factors, the ambient density, and/or the initial mass of the shells, the observed variability values are not recovered. Therefore, the central engine seems to play a relevant role in the explanation for the observed correlation. In fact, this correlation was also explored within the context of a model in which the GRB variability is due to a change in the jet-opening angles and narrower jets have faster outflows [156]. As a result, this model predicts bright luminosities, small pulse lags, and large variability as well as an early jet break time for on-axis observed bursts. On the other hand, dimmer luminosities, longer pulse lags, flatter bursts, and later jet break times will cause larger viewing angles.

Guidorzi et al. [151] gave an interpretation for the smaller value of the correlation in the context of the jet-emission scenario where a stronger dependence of of the expanding shells on the jet-opening angle is expected. However, Schaefer [157] attributed the origin of the relation to be based on relativistically shocked jets. Indeed, and are both functions of , where is proportional to a high power of , as was already demonstrated in the context of the relation (see Section 3.1.2), and hence fast rise times and short pulse durations imply high variability.

##### 3.3. The Correlation and Its Physical Interpretation

Schaefer [158] predicted that should be connected with in a following manner:with the exponent (see also Schaefer [157, 158]). Therefore, fast rises indicate high luminosities and slow rises low luminosities. can be directly connected to the physics of the shocked jet. Indeed, for a sudden collision of a material within a jet (with the shock creating an individual pulse in the GRB light curve), will be determined as the maximum delay between the arrival time of photons from the center of the visible region versus their arrival time from its edge.

The angular opening of the emitted jet, usually associated with , could cause this delay leading to a relation . The radius at which the material is shocked affects the proportionality constant, and the minimum radius under which the material cannot radiate efficiently anymore should be the same for each GRB [139]. In addition, a large scatter is expected depending on the distance from which the collisions are observed.

With both and being functions of , Schaefer [157] confirmed that should be . From 69 GRBs detected by BATSE and* Swift*, the following relation was obtained:

with in and measured in seconds. The uncertainties in the intercept and slope are and (see Figure 4(a)). The uncertainty in the log of the burst luminosity iswhere Schaefer [157] takes into account the extra scatter, . When , of the best-fit line is unity.

**(a)**

**(b)**

Xiao and Schaefer [159] explained in detail the procedure of how they calculated using 107 GRBs with known spectroscopic redshift observed by BATSE,* HETE*,* KONUS*, and* Swift* (see Figure 4(b)), taking into account also the Poissonian noise. Their analysis yieldedwith the same units as in (23). As a consequence, the flattening of the light curve before computing the rise time is an important step. The problem is that the flattening should be done carefully, in fact if the light curve is flattened too much, a rise time comparable with the smoothing-time bin is obtained, while if it is flattened not enough, the Poissonian noise dominates the apparent fastest rise time, giving a too small rise time. Therefore, for some of the dimmest bursts, the Poissonian-noise dominant region and the smoothing-effect dominant region can coincide, thus not yielding values for the weakest bursts. Finally, the physical interpretation of this correlation is given by Schaefer [157]. It is shown that the fastest rise in a light curve is related to the Lorentz factor simply due to the geometrical rise time for a region subtending an angle of , assuming that the minimum radius for which the optical depth of the jet material is of order of unity remains constant. The luminosity of the burst is also a power law of , which scales as for . Therefore, the and the relations together yield the observed relation.

##### 3.4. The and Correlations and Their Physical Interpretation

Freedman and Waxman [160] in their analysis of the GRB emission, considering a relativistic velocity for the fireball, showed that the radiation detected by an observer is within an opening angle . Hence, the total fireball energy should be interpreted as the energy that the fireball would have carried if this is assumed spherically symmetric. In particular, it was claimed that the afterglow flux measurements in X-rays gave a strong evaluation for the fireball energy per unit solid angle represented by , within the observable opening angle , where is the electron energy fraction. It was found thatwhere is in units of , is the uniform ambient density of the expanding fireball in units of , and is the time of the fireball expansion in days. Finally, it was pointed out that from the afterglow observations should be close to equipartition, namely, . For example, for GRB970508, it was found that [161–163]. A similar conclusion, that is, that it is also close to equipartition, could be drawn for GRB971214; however Wijers and Galama [162] proposed another interpretation for this GRB’s data, demanding .

Liang et al. [164] selected from the* Swift* catalogue 20 optical and 12 X-ray GRBs showing the onset of the afterglow shaped by the deceleration of the fireball due to the circumburst medium. The optically selected GRBs were used to fit a linear relation in the plane, where is the initial Lorentz factor of the fireball and is in units of (see Figure 5(a)). The best-fit line of the relation is given bywith , , and which can be measured with the deviation of the ratio . It was found that most of the GRBs with a lower limit of are enclosed within the region represented by the dashed lines in Figure 5(a), and it was pointed out that GRBs with a tentative derived from RS peaks or the afterglow peaks, as well as those which lower limits of were derived from light curves with a single power law, are systematically above the best-fit line. The lower values of , obtained from a set of optical afterglow light curves with a decaying trend since the start of the detection, were compatible with this correlation.

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Later, this correlation was verified by Ghirlanda et al. [165] and Lü et al. [143]. Ghirlanda et al. [165], studying the spectral evolution of 13 SGRBs detected by* Fermi*/GBM, investigated spectra resolved in the 8 keV–35 MeV energy range, and confirmed the results of Liang et al. [164].

Lü et al. [143] enlarged this sample reaching a total of 51 GRBs with spectroscopically confirmed redshifts and engaged three methods to constrain : the afterglow onset method [166] which considers of the early afterglow light curve as the deceleration time of the external FS; the pair opacity constraint method [167] which requires that the observed high-energy -rays (i.e., those in the GeV range) are optically thin to electron-positron pair production, thus leading to a lower limit on of the emitting region; the early external forward emission method [168] where an upper limit of can be derived from the quiescent periods between the prompt emission pulses, in which the signal of external shock has to go down the instrument thresholds. Considering some aspects of the external shock emission, the correlation was statistically reanalysed using 38 GRBs with calculated using method (as the other two provide only a range of the Lorentz factors, not a definite value), findingwith , and in units of . In addition, applying the beaming correction, a relation between and , using the same sample (see Figure 5(b)), was found to bewith and in units of .

Regarding the physical interpretation, Liang et al. [164] claimed that this correlation clearly shows the association of with angular structure, and this result yielded another evidence for the fireball deceleration model. Instead, Lü et al. [143] found that this relation is well explained by a neutrino-annihilation-powered jet during the emission, indicating a high accretion rate and not very fast BH spin. Besides, evidence for a jet dominated by a magnetic field have already been presented [169–171]. From the studies of the BH central engine models it was also indicated that magnetic fields are a fundamental feature [172]. Nevertheless, the baryon loading mechanism in a strongly magnetized jet is more complex, and it has still to be fully investigated.

##### 3.5. Correlations between the Energetics and the Peak Energy

###### 3.5.1. The and the Correlations

Mallozzi et al. [110] analysed 399 GRBs observed by BATSE and discovered a correlation between the logarithmic average peak energies and . Choosing as a selection criterion for the bursts , they derived from the count rate data in time bins in the energy band and used the distribution derived from the Comptonized photon model (the differential photon number flux per unit energy):with the normalization, the spectral index, and . Then, they grouped the sample into 5 different width bins of about 80 events each (see Figure 6). The bursts were ranked such that group 1 had the lowest peak flux values and group 5 had the highest values. They found a correlation with and . Lower intensity GRBs exhibited a lower .

Later, Lloyd et al. [173] examined the correlation with 1000 simulated bursts in the same energy range as Mallozzi et al. [110] and found a strong correlation between and (see Figure 7(a)). The relation between the two variables was as follows:with the Kendall correlation coefficient [174] and . In addition, they compared it to the relation (see Figure 7(b)). This relation was for the whole spectral sample and consistent with earlier results [110, 175]. However, they selected a subsample composed of only the most luminous GRBs, because spectral parameters obtained from bursts near the detector threshold are not robust. Therefore, to better understand the selection effects relevant to and burst strength, they considered the following selection criteria: , , and . Due to the sensitivity over a certain energy band of all the detectors, especially BATSE, and to some restrictions to the trigger, the selection effects are inevitable. However, the subsample of the most luminous GRBs presents a weak correlation. Instead, a tight correlation was found for the whole sample as well as the subsample of the brightest GRBs. Lloyd et al. [173] paid more attention to the correlation for the brightest GRBs because it is easier to deal with the truncation effects in this case, and the cosmological interpretation is simpler.

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This correlation has been the basis for the investigation of the Amati relation (see Section 3.5.2) and the Ghirlanda relation (see Section 3.5.3). Lloyd et al. [173] concluded that “the observed correlation can be explained by cosmological expansion alone if the total radiated energy (in the -ray range) is constant.” In fact, their finding does not depend on the GRB rate density or on the distribution of other parameters. However, the data from GRBs with known redshift are incompatible with a narrow distribution of radiated energy or luminosity.

Following a different approach, Goldstein et al. [176] pointed out that the ratio can serve as an indicator of the ratio of the energy at which most of the -rays are radiated to the total energy and claimed that the relation is a significant tool for classifying LGRBs and SGRBs. The fluence indicates the duration of the burst without providing a biased value of and displays, as a spectral hardness ratio, an increased hardness for SGRBs in respect to LGRBs, in agreement with [10]. This correlation is quite interesting, since the energy ratio, being dependent only on the square of the luminosity distance, gets rid of the cosmological dependence for the considered quantities. Therefore, it was evaluated that the energy ratio could be used as a GRB classifier.

Later, Lu et al. [177], with the results of time-resolved spectral analysis, computed the relation for 51 LGRBs and 11 bright SGRBs observed with* Fermi*/GBM. For each GRB, they fitted a simple power law function. They measured its scatter with the distance of the data points from the best-fit line. The measured scatter of the relation is . This result was reported for the first time by Golenetskii et al. [178] and later confirmed by Borgonovo and Ryde [179]; Ghirlanda et al. [180]; Guiriec et al. [181]; Ghirlanda et al. [165].

###### 3.5.2. The Correlation

Evidence for a correlation between and was first found by Lloyd and Petrosian [182] and Lloyd et al. [183] based on 46 BATSE events, but this relation was in the observer frame due to the paucity of the data with precise redshift measurement, as was shown in previous paragraphs. Evidence for a stronger correlation between and , also called the Amati relation, was reported by Amati et al. [111] based on a limited sample of 12 GRBs with known redshifts (9 with firm redshift and 3 with plausible values) detected by* BeppoSAX*. They found thatwith , , and calculated asRegarding the methodology considered, instead of fitting the observed spectra, as done, for example, by Bloom et al. [184], the GRB spectra were blue-shifted to the rest frames to obtain their intrinsic form. Then, the total emitted energy is calculated by integrating the Band et al. [115] spectral model in energy band and scaling for the luminosity distance. This was computed employing a flat Friedmann-Lemaitre-Robertson-Walker cosmological model with , , and taking into account both the cosmological time dilation and spectral redshift.

Amati et al. [185] enlarged the set of Amati et al. [111] by including 20 GRBs from* BeppoSAX* with known redshift for which new spectral data (*BeppoSAX* events) or published best-fitting spectral parameters (BATSE and* HETE-2* events) were accessible. The relation was found to bewith , , in keV and in units of . Therefore, its statistical significance increased, providing a correlation coefficient comparable to that obtained by Amati et al. [111], but based on a larger set.

Based on* HETE-2* measurements, Lamb et al. [186] and Sakamoto et al. [187] verified the previous results and considered also XRFs, finding out that the Amati relation remains valid over three orders of magnitude in and five orders of magnitude in . The increasing amount of GRBs with measured redshift allowed verifying this relation and strengthen its validity, as found by Ghirlanda et al. [188] with 29 events ( and ; see Figure 9(a)).

Ghirlanda et al. [189] verified the correlation among LGRBs considering a set of 442 BATSE GRBs with measured and with pseudoredshifts computed via the correlation. It was shown that the scatter of the sample around the best-fitting line is comparable with that of another set composed of 27 GRBs with measured spectroscopic redshifts. This is because the weights of the outliers were marginal. It was noted that the relation for the 442 BATSE GRBs has a slope slightly smaller (0.47) than the one obtained for the 27 GRBs with measured spectroscopic redshifts (0.56).

Afterwards, Amati [190] (see Figures 8(a) and 8(c)) updated the study of the correlation considering a sample of 41 LGRBs/XRFs with firm values of and , 12 GRBs with uncertain and/or , 2 SGRBs with certain values of and , and the subenergetic events GRB980425/SN1998bw and GRB031203/SN2003lw. The different sets are displayed in Figure 8(b). Taking into account also the sample variance, it was found thatwith , , and units being the same as in (34). Moreover, subenergetic GRBs (980425 and possibly 031203) and SGRBs were incompatible with the relation, suggesting that it can be an important tool for distinguishing different classes of GRBs. Indeed, the increasing number of GRBs with measured and can provide the most reliable evidence for the existence of two or more subclasses of outliers for the relation. Moreover, the relation is valid also for the particular subenergetic event GRB060218. Finally, the normalization considered by Amati [190] is consistent with those obtained by other instruments.

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Ghirlanda et al. [191] confirmed the correlation for softer events (XRFs). The sample consisted of 76 GRBs observed by several satellites, mainly* HETE-2*,* KONUS*/Wind,* Swift*, and* Fermi*/GBM. The most important outcome is a tight correlation with no new outliers (with respect to the classical GRB980425 and GRB031203) in the plane. The obtained relation was

Amati et al. [192] studied 95* Fermi* GRBs with measured and obtained an updated relation, which readwith and . In particular, they investigated two GRBs (080916C and 090323) with very energetic prompt emission and found that they follow the relation well. On the other hand, an SGRB, 090510, also a very luminous and energetic event, was found not to obey the relation. Hence, Amati et al. [192] proposed that the correlation might serve as a discriminating factor among high-energetic GRBs. In addition, they claimed that the physics of the radiation process for really luminous and energetic GRBs is identical to that for average-luminous and soft-dim long events (XRFs), because all these groups follow the Amati relation.

Later, Amati [193] provided an update of the analysis by Amati et al. [194] with a larger sample of 120 GRBs (see Figure 8(b)) finding it to be consistent with the following relation:with units the same as in (34) and (35). Afterwards, Qin and Chen [195] analysed a sample of 153 GRBs with measured , , , and , observed by various instruments up to 2012 May. The distribution of the logarithmic deviation of from the Amati relation displayed a clear bimodality which was well represented by a mixture of two Gaussian distributions. Moreover, it was suggested to use the logarithmic deviation of the value for distinguishing GRBs in the versus plane. This procedure separated GRBs into two classes: the Amati type bursts, which follow the Amati relation, and the non-Amati type bursts, which do not follow it. For the Amati type bursts it was found thatwith and , while, for non-Amati bursts,with and . In both relations is in keV, and is in units of .

In addition, it was pointed out that almost all Amati type bursts are LGRBs at higher energies, as opposed to non-Amati type bursts which are mostly SGRBs. An improvement to this classification procedure is that the two types of GRBs are clearly separated; hence different GRBs can be easily classified.

Heussaff et al. [196], applying particular selection criteria for the duration and the spectral indices, obtained a set of* Fermi* GRBs and analysed their locations in the plane. The sample, composed of 43 GRBs with known redshifts, yielded the following relation:with , , and the same units as in previous relations of this type.

Amati and Della Valle [197] pointed out that an enlarged sample of 156 LGRBs with known and also follows the Amati relation with a slope (see Figure 8(d)). Additionally, Basak and Rao [198] showed that a time-resolved Amati relation also holds within each single GRB with normalization and slope consistent with those obtained with time-averaged spectra and energetics/luminosity and is even better than the time-integrated relation [199]. Time-resolved and are obtained at different times during the prompt phase (see also [177, 180, 200] and Section 3.6).

###### 3.5.3. The Correlation

The relation (also called the Ghirlanda relation) was first discovered by Ghirlanda et al. [188], who used 40 GRBs with and known at their time of writing. Considering the time , its value can be used to deduce from . Indeed, even if only a little less than half of the bursts have observed jet breaks (47%), from [107] we know thatwhere is measured in days, is the density of the circumburst medium in particles per , is the radiative efficiency, and is in units of . Here, is in degrees and it is the angular radius (the half opening angle) subtended by the jet. For GRBs with no measured , the median value of the distribution of the computed densities, extending between 1 and , was considered [139, 201–203].

Later, Liang and Zhang [204] using a sample of 15 GRBs with measured , and , considered a purely phenomenological of the optical afterglow light curves, thus avoiding the assumption of any theoretical model, contrary to what was done by Ghirlanda et al. [188]. The functional form of this correlation is given by:where is in units of , in units of , is measured in days, and and .

Nava et al. [205] found that the Ghirlanda relation, assuming a wind-like circumburst medium, is as strong as the one considering a homogeneous medium. They analysed the discrepancy between the correlations in the observed and in the comoving frame (with Lorentz factor identical to the fireball’s one). Since both and transform in the same way, the wind-like Ghirlanda relation remains linear also in the comoving frame, no matter what the Lorentz factor’s distribution is. The wind-like relation corresponds to bursts with the same number of photons emitted. Instead, for the homogeneous density medium scenario, it is common to consider a tight relation between the Lorentz factor and the total energy, thus limiting the emission models of the prompt radiation. Using 18 GRBs with firm , , and , Nava et al. [205] found for the homogeneous density casewith and . Instead, for the wind casewith and .

Ghirlanda et al. [206] tested the correlation using 33 GRBs (16 new bursts detected by* Swift* with firm and up to December 2006, and 17 pre-*Swift* GRBs). They claimed that, for computing , the following is required:(1)The detection of the jet break should be in the optical.(2)The optical light curve should continue up to a time longer than the .(3)The host galaxy flux and the flux from a probable SN should be removed.(4)The break should not depend on the frequency in the optical, and a coincident break in the X-ray light curve is not necessary, because the flux in X-rays could be controlled by another feature.(5)The considered should be different from the one at the end of the plateau emission (the time in [81]); otherwise the feature affecting the X-ray flux is also influencing the optical one.

Therefore, considering all these restrictions, the sample was reduced to 16 GRBs, all compatible with the following relation:No outliers were detected. Therefore, the reduced scatter of the relation corroborates the use of GRBs as standardizable candles.

###### 3.5.4. Physical Interpretation of the Energetics versus Peak Energy Relations

Lloyd et al. [173] investigated the physical explanation of the correlation assuming the emission process to be a synchrotron radiation from internal and external shocks. Indeed, they claimed that this correlation is easily obtained considering a thin synchrotron radiation by a power law distribution of electrons with larger than some minimum threshold value, . Moreover, the internal shock model illustrates the tight relation and the emitted energy better than the external shock model.

Lloyd-Ronning and Petrosian [207] pointed out that the GRB particle acceleration is not a well analysed issue. Generally, the main hypothesis is that the emitted particles are accelerated via recurrent scatterings through the (internal) shocks. They found that the recurrent crossings of the shock come from a power law distribution of the particles with a precise index, providing a large energy synchrotron photon index. Moreover, the connection between and the photon flux can be justified by the variation of the magnetic field or electron energy in the emission events. Finally, they claimed that, in the majority of GRBs, the acceleration of particles is not an isotropic mechanism but occurs along the magnetic field lines.

Amati et al. [111] confirmed the findings of Lloyd et al. [183] that the relation is obtained assuming an optically thin synchrotron shock model. This model considers electrons following the distribution for with , GRB duration, and constant in each GRB. However, the above assumptions are not fully justifiable. In fact the duration is different in each GRB and might be smaller in the case of beamed emission.

Amati [190] pointed out the impact that the correlation has on the modeling of the prompt emission and on the possible unification of the two classes of GRBs and XRFs. In addition, this correlation is often applied for checking GRB synthesis models (e.g., [208, 209]).

In every model, and depend on , and the relation can help to relate the parameters of the synchrotron shock model and inverse-Compton model [203, 208]. Specifically, Zhang and Mészáros [208] and Rees and Mészáros [210] found that, for an electron distribution given by a power law and produced by an internal shock in a fireball with velocity , the peak energy is given aswhere is the total fireball luminosity and is the variability timescale. However, to recover the relation from this relation, and should be similar for each GRB, a condition that cannot be easily supported. A further issue arises when one considers that , with between 2 and 3 in different models [203, 208, 211]. An explanation could be that direct or Comptonized thermal radiation from the fireball photosphere [208, 210–219] can affect significantly the GRB prompt emission. This can be a good interpretation of the really energetic spectra presented for many events [220–222] and the flat shape in GRB average spectra. In such cases, depends on the peak temperature of photons distributed as by a blackbody, and therefore it is associated with the luminosity or emitted energy. For Comptonized radiation from the photosphere the relations areorwhere is a particular distance between the central engine and the energy radiating area, such that the Lorentz factor evolves as up to some saturation radius [210]. As suggested by Rees and Mészáros [210], in this scenario the relation could be recovered for particular physical cases just underneath the photosphere, though it would rely on an undefined number of unknown parameters.

Also for high-energetic GRBs (i.e., ) the nonthermal synchrotron emission model can explain the correlation. This can be possible by considering either the minimum Lorentz factor and the normalization of the power law distribution of the emitting electrons constant in each GRB or constraints on the slope of the relation between and the luminosity [183, 208].

Panaitescu [223] used 76 GRBs with measured redshifts to analyse the case in which the relation for LGRBs is due to the external shock generated by a relativistic outflow interacting with the ambient medium. He considered the effect of each parameter defining the relation on the radial distribution of the external medium density and pointed out that the relation is recovered if the external medium is radially stratified. For some combinations of radiative (synchrotron or inverse-Compton) and dissipation (such as RS or FS) mechanisms, it is concluded that the external medium requires a particle density distributed distinctly from , with being the distance at which the GRB radiation is generated. This tendency should be commonly associated with uniform mass-loss rate and final velocity.

Mochkovitch and Nava [224] checked whether the relation can be recovered in a case when the prompt emission is due to internal shocks, or alternatively if the correlation can give some limits for the internal shock scenario defined through the impact of only two shells. Simulated GRB samples were obtained considering different model parameter distributions, such as the emitted power in the relativistic emission and . Simulated distributions were plotted for each case and analysed together with the observed relation (based on 58 GRBs). The sample contained only luminous* Swift* GRBs with in the energy band. In conclusion, a correspondence between the model and data was found, but exclusively if the following restrictions for the dynamics of the emission and for the dispersion of the energy are assumed:(1)The majority of the dispersed energy should be radiated in few electrons.(2)The spread between the highest and the lowest Lorentz factor should be small.(3)If the mean Lorentz factor grows as (where is the rate of injected energy, or mean emitted power, in the relativistic outflow), the relation is not retrieved and is diminishing with larger . However, the relation can be regained if is a lower constraint for a particular .(4)When the timescale or the width of the variability of the Lorentz factor is associated with , relation is recovered.

For the Ghirlanda relation [188], with the assumption that the line of sight is within the jet angle, the relation indicates its invariance when moving from the rest frame to the comoving frame. As a result, the number of radiated photons in each GRBs is comparable and should be about . The last characteristic could be important for understanding the dynamics of GRBs and the radiative mechanisms (see also Figure 9(b)).

Collazzi et al. [225] found that the mean is near to , the electron rest-mass energy . Therefore, it is claimed that the tight shape of the distribution does not stem only from selection effects. No studied mechanism can drive this effect; however, with the compatible with the effective temperature of the -ray radiating area, the almost constant temperature needs some mechanism similar to a thermostat, keeping the temperature at a steady value. It was suggested that such a mechanism could be an electron-positron annihilation.

Ghirlanda et al. [209], using a simulated sample, analysed if different intrinsic distributions of and can replicate a grid of observational constraints. With the assumption that, in the comoving frame each GRB has similar and , it was found that the distributions of and cannot be power laws. Instead, the highest concordance between simulation and data is given by log-normal distributions and a connection between their maxima, like . In this work and are important quantities for the calculation of the GRB energetics. Indeed, from a sample of ≈30 GRBs with known or it was found that the distribution is centered at and it is tightly related to . It was obtained that

Present values of and rely on incomplete data sets and their distributions could be affected by biases. Nevertheless, Ghirlanda et al. [209] claimed that greater values of are related to smaller values; that is, the faster a GRB, the narrower its jet.

Furthermore, GRBs fulfilling the condition might not display any jet break in the afterglow light curve, and Ghirlanda et al. [209] predicted that this group should comprise ≈6% of the on-axis GRBs. Finally, their work is crucial as it allowed finding that the local rate of GRBs is ≈0.3% of the local SNe Ib/c rate and ≈4.3% of the local hypernovae (i.e., SNe Ib/c with wide-lines) rate.

##### 3.6. Correlations between the Luminosity and the Peak Energy

###### 3.6.1. The Correlation

The relation was discovered by Schaefer [203] who used 84 GRBs with known from the BATSE catalogue [121] and 20 GRBs with luminosities based on optically measured redshift [111, 226]. It was found that (see Figure 10) for the 20 GRBswith and , and among the 84 GRBs the relation wasThe underlying idea is that varies as a power of , as we have already discussed in Section 3.1.2, and also varies as some other power of , so that and will be correlated to each other through their dependence on . For the general case where the luminosity varies as and varies as , and therefore will vary as .

Frontera et al. [200], using a sample of 9 GRBs detected simultaneously with the Wide Field Camera (WFC) on board the* BeppoSAX* satellite and by the BATSE instrument, reported the results of a systematic study of the broadband () time-resolved prompt emission spectra. However, only 4 of those GRBs (970111, 980329, 990123, 990510) were bright enough to allow a fine time-resolved spectral analysis, resulting in a total of 40 spectra. Finally, the study of the time-resolved dependence (see also the end of Section 3.5.2) of on the corresponding was possible for two bursts with known redshift (i.e., 990123 and 990510) and found using the least squares method (see Figure 11):with and .

Afterwards, Nava et al. [227], using a sample of 46* Swift* GRBs with measured and , found a strong correlation, with a functional form of