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Advances in High Energy Physics

Volume 2014, Article ID 469572, 10 pages

http://dx.doi.org/10.1155/2014/469572
Research Article

Residual Symmetries Applied to Neutrino Oscillations at NOA and T2K

1Department of Physics and Astronomy, Michigan State University, East Lansing, MI 48824, USA

2Department of Physics and Center for Particles and Fields, University of Texas, Austin, TX 78712, USA

Received 3 April 2014; Accepted 24 July 2014; Published 24 August 2014

Academic Editor: Hiro Ejiri

Copyright © 2014 Andrew D. Hanlon et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The publication of this article was funded by SCOAP3.

Abstract

The results previously obtained from the model-independent application of a generalized hidden horizontal symmetry to the neutrino mass matrix are updated using the latest global fits for the neutrino oscillation parameters. The resulting prediction for the Dirac phase is in agreement with recent results from T2K. The distribution for the Jarlskog invariant has become sharper and appears to be approaching a particular region. The approximate effects of matter on long-baseline neutrino experiments are explored, and it is shown how the weak interactions between the neutrinos and the particles that make up the Earth can help to determine the mass hierarchy. A similar strategy is employed to show how NOA and T2K could determine the octant of . Finally, the exact effects of matter are obtained numerically in order to make comparisons with the form of the approximate solutions. From this analysis there emerge some interesting features of the effective mass eigenvalues.

1. Introduction

Although there has been significant progress in neutrino physics from oscillation experiments, there remains much work to be done. The reactor angle has now been measured to greater accuracy than ever before, and the solar angle has been known for some time now. But, the octant of the atmospheric angle ( or ) or whether this angle is maximal () has yet to be answered. Determination of the Dirac phase has been improved. Recent results from T2K exclude at C.L. for normal hierarchy (NH) and for inverted hierarchy (IH) [1]. Finally, the absolute value of the mass squared differences has been carefully measured, but the mass hierarchy is still undetermined (i.e., or ). Each of these questions will be discussed in this work.

From the improvements in recent global analyses [24] it is possible to make more accurate predictions for the distributions of some of the aforementioned parameters of interest. Specifically, each of the residual symmetries, and , can be used to derive a model-independent equation for (one for each symmetry) [5, 6]. Then using the newly available global fits of the neutrino oscillation parameters in [2], likelihood distributions for , the Jarlskog invariant [7], and are obtained.

Using the PMNS mixing matrix, an expression for the probability of a neutrino originally of flavor to be detected as a neutrino of flavor , is presented (which is a standard result found in many review papers on neutrino physics [8]). Then, using the approximation from [9] it is shown how the earth’s matter affects the neutrino beam in long-baseline experiments. This is done by replacing the oscillation parameters with effective values that depend on the energy of the neutrinos, the baseline length, and the density of the matter.

In this paper, a focus is made on the NOA and T2K experiments. Both of these experiments measure the appearance of ’s (’s) from a beam. The probability for this appearance is plotted as a function of energy using the best fits for the oscillation parameters in [2]. The effects of matter are taken into account using the average matter density along the baseline for the two experiments. This is justified by the fact that there does not appear to be a significant effect due to the variation of the matter density [10]. A comparison is made for this probability with and without -violation in an attempt to observe the sensitivity of NOA and T2K to measurements of . We have also plotted versus which shows that it may be possible for these experiments to determine the neutrino mass hierarchy for some values of the phase as discussed in [11, 12].

The update of the analysis of [13] given in [2] gives closer agreement on with the other two major global analyses [3, 4]. This shows that is closer to being maximal than originally believed and only excludes the possibility of it being maximal by about for inverted hierarchy. But, it is clear that the analyses do not agree upon which octant is favored. Fortunately, the plots of versus may also serve to determine the octant of [11, 12].

This work is concluded with a digression into the effective mixing angles and masses in matter. The solar resonance, first described by the MSW effect [1416], and the atmospheric resonance are readily observed.

2. Distribution of , , and

The equations for , in terms of the neutrino mixing angles, based on residual symmetries are given by [5, 6] for and respectively, where and . The latest global fits for the neutrino oscillation parameters from [2] are shown in Table 1.

tab1
Table 1: Global fits for neutrino oscillation parameters from [2]. * represents a local minimum at approximately for .

From this we can obtain a distribution for following the procedure in [5, 6] by using where , the ’s are proportional to , and RHS of (1a), (1b). Because it is preferable to get a distribution with respect to rather than we use where and . Since this is a numerical integral, the delta function cannot be used as it is normally defined (unless integrated out of the equation prior to the numerical calculation). The integral was evaluated using a Monte Carlo algorithm and the results are shown in Figure 1(a). The domain of in (3) is , but the distributions in Figure 1(a) can be reflected about to account for the full interval . Therefore, these distributions have been normalized to over the domain shown in the figures. This means that each of the residual symmetries will have two peak predictions for the phase (equidistant from ). The IH curve for in [2] is closer to being symmetric about . This is very prevalent in the results shown in Figure 1(a) given that the IH plots are close to being symmetric about . But, since the NH global fit favors the lower octant for by at least [2] the predicted distributions for NH tend to prefer one side of . But in both cases the results for are in agreement with the best fit value of from T2K’s latest results [1].

fig1
Figure 1: Predicted distributions for (a) , (b) , and (c) (NH) using the global analysis in [2].

The same method is applied to the Jarlskog invariant [7]; that is, with . This distribution is shown in Figure 1(b). When calculating these distributions, is taken to be in the interval and is even about the vertical axis to extend to include . To account for this, the figures are labeled for the distribution of , and they can therefore be normalized to one. As compared with our previous results in [6], is beginning to favor the region that prefers. Also, the region predicted by has become slightly narrower and it now excludes .

Finally, this method is again applied similarly to by first using (1a), (1b) to solve for for and , respectively. Then we have with , where RHS of (5a), (5b). To get a distribution for we use The distribution is shown in Figure 1(c), where plots are made with and without using the prior on from [2]. When no prior on is used, becomes evenly distributed in . As previously discussed in [6], is symmetric about when there is no prior on . In addition, the distributions using the prior on have also become more symmetric, as a result of the for also having become more symmetric about zero.

3. to Oscillation

Now that we have a distribution for all the neutrino oscillation parameters, an attempt can be made to predict the results of an experiment measuring the number of ’s that oscillate into ’s over some distance. First, the expression for this probability, , must be found. Denoting the weak eigenstates of the neutrino by and the neutrino mass eigenstates by , then defines the PMNS mixing matrix, . The standard parametrization is given by [9] where From [8], which leads to where , is the th mass eigenvalue, is the distance propagated by the neutrino, and is the energy of the neutrino. Notice that this probability does not depend on the Majorana phases, and therefore a discussion on these phases will not be pursued here.

Making the following definition [9]: and noting that , then The last term includes the Jarlskog invariant [7] defined above.

3.1. Matter Effects

As electron neutrinos propagate through the earth, they can interact with electrons via -exchange. In addition, all three neutrino flavors can interact with electrons, protons, or neutrons via -exchange. Assuming electrically neutral matter, the -exchange between the neutrinos and protons will exactly cancel with the -exchange between the neutrinos and electrons [8]. The contribution from -exchange can be dropped, because it only adds a multiple of the identity matrix to the Hamiltonian [9]. Then, under the assumption that , the effect of -exchange can be accounted for by modifying the Hamiltonian for neutrinos [17] where and is the density of electrons. For antineutrinos, the Hamiltonian is simply the complex conjugate of (15) with .

One way to proceed is to diagonalize the Hamiltonian exactly, which has been done analytically [1719]. However, this does not give much physical insight into the effects of matter on neutrino oscillations. Approximations in which the mixing angles and mass eigenvalues are replaced by effective values do not modify any of the equations, and therefore it becomes clear how matter affects neutrinos. A number of approximation schemes have been developed [2026]. One of the most commonly used of these are the equations derived in [26]. But, due to the large value of measured at Daya Bay [27], the approximation in [26] begins to fail as is shown in [9]. In the approximation that is used here, the form of (14) can be used with the following modifications [9]: with where for neutrinos let and for antineutrinos let with the upper sign for normal hierarchy and the lower sign for inverted hierarchy.

It is helpful to show and in conventional units. Following [9]

3.2. NOA and T2K

NOA is a long-baseline neutrino oscillation experiment located in northern Minnesota. It has a baseline length of 810 km, an average matter density of 2.8 g/cm3 along this baseline, and a peak neutrino energy around 2 GeV [11]. T2K is another neutrino oscillation experiment with similar goals to that of NOA. Its baseline length is 295 km and has an average matter density of 2.6 g/cm3, and the neutrino beam energy peaks around 0.6 GeV [28].

With the use of the effective mixing angles derived in the previous section, the probability of the appearance of a from a beam can be determined for any matter density. Using the length and matter density for the two experiments in question, plots of these probabilities are shown in Figure 2 as a function of energy.

fig2
Figure 2: as a function of energy at (a) NOA and (b) T2K, using the best fits from [2] with normal hierarchy.

It is not entirely apparent that the approximation [9] is valid for different values of the phase or the vacuum mixing angles; therefore, a comparison is made between this approximation and the exact results in the Appendix. In this comparison, the exact results are found by numerically diagonalizing the Hamiltonian. As it turns out, the approximation is very good for the energies and densities considered here.

4. Determination of the Mass Hierarchy and the Octant of

As has been mentioned previously, a major goal of neutrino oscillation experiments is to determine the mass hierarchy. If was a good symmetry, then there would be no observable difference between and when the neutrinos are propagating through a vacuum. However, interestingly enough, the matter effects discussed previously emulate the effects of -violation. Therefore, there is an observable difference between and even if is a good symmetry. Without the effects of matter the difference between oscillation probabilities for normal hierarchy versus inverted hierarchy is minimal. Thus it is because of the interactions with matter that allow for a discernible difference between normal and inverted hierarchy.

It is possible that actual -violation is substantially cancelled by this matter induced -violation. This would be very unfortunate, because it would make the determination of the phase more difficult than expected. A plot for versus is shown in Figure 3 for NOA and T2K using the best fits from [2]. It can be seen that there are many values of the phase that will allow NOA to make a serious determination of the true mass hierarchy. This will occur if with NH being the true hierarchy or with IH being the true hierarchy. And since T2K has excluded most of at C.L. [1], hopefully the true mass hierarchy is normal. From Figure 3(b) it appears that T2K will not be able to determine the mass hierarchy in this manner.

fig3
Figure 3: Plot of versus to show the sensitivity of (a) NOA and (b) T2K to determine the mass hierarchy assuming . The red ellipse (lower right corner) corresponds to NH, and the blue ellipse (upper left corner) corresponds to IH.

In addition, it may also be possible to determine the octant of from similar plots. These are shown in Figure 4. It appears that every value of the phase could at least give some indication of the true octant of , but the best values would be for the lower octant and for the higher octant.

fig4
Figure 4: Plot of versus to show the sensitivity of (a) NOA and (b) T2K to determine the octant of assuming inverted hierarchy. The red ellipses (lower left corner) correspond to , while the blue ellipses (upper right corner) correspond to . The dashed ellipses correspond to the values.

The ellipses were created by using (14) with the matter effect modifications of (16), for all possible values of (i.e., ). The and the symbols correspond to the predicted values for , based on and , respectively. The predicted values are determined by using the best fits from [2] in (1a), (1b).

5. Effective Masses and Mixing Angles in Matter

The values of the effective mixing angles are plotted in Figure 5 and the mass eigenvalues in Figure 6, as functions of energy using the matter density for the NOA experiment. The plots for T2K are excluded here, because they do not differ much from the ones for NOA. Also, these particular plots consider , because the results depend very little on the phase. These have been plotted by numerically diagonalizing the Hamiltonian. It is assumed that the diagonalization matrix will have the same form as the standard parameterization of the PMNS mixing matrix.

fig5
Figure 5: Plots of the effective mixing angles as a function of energy using data from [2]. For (a) NOA and neutrinos, (b) NOA and antineutrinos. Red , blue , and green . The solid lines are for normal hierarchy, and the dashed lines are for inverted hierarchy. In the cases where the dashed line is not visible, it’s because the solid line is on top of it.
fig6
Figure 6: Effective masses for NOA. The major focus of these plots should be on the solar and atmospheric resonances corresponding to a level repulsion. (a) and NH, (b) and IH, (c) and NH, and (d) and IH. Red , blue , green , cyan-dashed , and magenta-dashed .

The approximation introduced in Section 3.1 implies that the phase and do not vary much, if at all, due to interactions with matter (which can be observed in Figure 5). It also implies certain characteristics of the variations of the other two mixing angles. From (17a), should be independent of the mass hierarchy, and taking the limit , then () for (). This behavior is easily observed in Figure 5. From (17b), should have similar asymptotic behavior as for normal hierarchy, while it should reverse its behavior for inverted hierarchy. These features are approximately shown in Figure 5, but at the energies shown, is not able to approach its asymptotic limit. Therefore, these results appear to agree with the approximation in [9].

The effective neutrino masses are found from multiplying the eigenvalues of the Hamiltonian by . These plots are shown in Figure 6 for NOA. There are some interesting characteristics of these plots. The first and most obvious are two resonances referred to as the solar resonance and the atmospheric resonance which represent the condition for maximal oscillation probability. This phenomenon was first understood with the introduction of the MSW effect [14, 15]. The first peak of is the solar resonance and corresponds to an approach of and followed by a repulsion. The first peak of is the atmospheric resonance and corresponds to an approach of and followed by a repulsion. If the absolute value of the mass eigenvalues crosses, then no resonance can be seen there. If we do not take the absolute value of the mass eigenvalues, then they will never cross each other. This is a wonderful example of level repulsion in quantum mechanics. For more details on these resonances, including a derivation of the resonance condition, see [1416, 29].

6. Conclusions

Predicted distributions for , , and were updated using the residual symmetries and . It was found that the greater uncertainty in the octant of for IH shown in [2] forced the distributions of for IH to have nearly equal contributions on either side of . This had no significant effect on the distribution for and the prediction for has improved.

By including the effects of matter into the oscillation probabilities, it was shown in Section 4 how NOA stands a good chance of determining the mass hierarchy if and the true hierarchy is normal or if and the true hierarchy is inverted. It was also shown that both NOA and T2K may be capable of nailing down the octant of .

The effects of matter were also shown to give rise to two resonances: the solar resonance and the atmospheric resonance. This behavior can be seen to agree with the approximation used throughout this work [9].

Appendix

Comparison with Solving for Matter Effects Exactly

Here a comparison is made between the approximation used [9] and exact results found from numerically diagonalizing the Hamiltonian. Each plot for and above has been redone without any approximation. The plots in Figure 7 show the difference between these two methods. It is clear that the approximation is indeed very good, with a maximum difference around .

fig7
Figure 7: Comparison between the exact results and the approximation used throughout the paper. For (a) NOA and neutrinos and (b) NOA and antineutrinos. Red , red-dash , green , green-dash: , blue: , and blue-dash: .

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

The authors would like to thank Shao-Feng Ge for the contributions in the early stages of this work. Wayne W. Repko would also like to thank Kendall Mahn for some helpful conversations. All plots in this paper were produced using matplotlib [30]. Wayne W. Repko was supported in part by the National Science Foundation under Grant no. PHY-1068020. Duane A. Dicus was supported in part by the U.S. Department of Energy under Award no. DE-FG02-12ER41830.

References

  1. K. Abe, J. Adam, H. Aihara et al., “Observation of electron neutrino appearance in a Muon neutrino beam,” Physical Review Letters, vol. 112, Article ID 061802, 2014. View at Publisher · View at Google Scholar
  2. F. Capozzi, G. Fogli, E. Lisi et al., “Status of three-neutrino oscillation parameters, circa 2013,” Physical Review D, vol. 89, Article ID 093018, 2013. View at Publisher · View at Google Scholar
  3. D. Forero, M. Tortola, and J. Valle, “Global status of neutrino oscillation parameters after Neutrino-2012,” Physical Review D, vol. 86, Article ID 073012, 2012. View at Publisher · View at Google Scholar
  4. M. Gonzalez-Garcia, M. Maltoni, J. Salvado, and T. Schwetz, “Global fit to three neutrino mixing: critical look at present precision,” Journal of High Energy Physics, vol. 2012, article 123, 2012. View at Publisher · View at Google Scholar
  5. S.-F. Ge, D. A. Dicus, and W. W. Repko, “Residual Symmetries for Neutrino Mixing with a Large theta_13 and Nearly Maximal delta_D,” Physical Review Letters, vol. 108, Article ID 041801, 2012. View at Publisher · View at Google Scholar
  6. A. D. Hanlon, S.-F. Ge, and W. W. Repko, “Phenomenological consequences of residual Z2s and Z2s symmetries,” Physics Letters B, vol. 729, pp. 185–191, 2014. View at Publisher · View at Google Scholar
  7. C. Jarlskog, “Commutator of the quark mass matrices in the standard electroweak model and a measure of maximal CP nonconservation,” Physical Review Letters, vol. 55, p. 1039, 1985. View at Publisher · View at Google Scholar
  8. B. Kayser, “Neutrino physics,” eConf C040802, L004, http://arxiv.org/abs/hep-ph/0506165.
  9. S. K. Agarwalla, Y. Kao, and T. Takeuchi, “Analytical approximation of the neutrino oscillation probabilities at large θ13,” http://arxiv.org/abs/1302.6773.
  10. M. Koike and J. Sato, “Effects of matter density fluctuation in long baseline neutrino oscillation experiments,” Modern Physics Letters A, vol. 14, no. 19, pp. 1297–1302, 1999. View at Publisher · View at Google Scholar
  11. R. Patterson, “The NOvA experiment: status and outlook,” Nuclear Physics B—Proceedings Supplements, vol. 235-236, pp. 151–157, 2013. View at Publisher · View at Google Scholar
  12. S. K. Agarwalla, S. Prakash, and S. U. Sankar, “Resolving the octant of θ23 with T2K and NOνA,” Journal of High Energy Physics, vol. 2013, article 131, 2013. View at Google Scholar
  13. G. L. Fogli, E. Lisi, A. Marrone, D. Montanino, A. Palazzo, and A. M. Rotunno, “Global analysis of neutrino masses, mixings and phases: entering the era of leptonic CP violation searches,” Physical Review D, vol. 86, Article ID 013012, 2012. View at Publisher · View at Google Scholar
  14. L. Wolfenstein, “Neutrino oscillations in matter,” Physical Review D, vol. 17, pp. 2369–2374, 1978. View at Google Scholar
  15. S. Mikheev and A. Y. Smirnov, “Resonant amplification of ν oscillations in matter and solar-neutrino spectroscopy,” Il Nuovo Cimento C, vol. 9, no. 1, pp. 17–26, 1986. View at Publisher · View at Google Scholar
  16. A. Y. Smirnov, “The MSW effect and matter effects in neutrino oscillations,” Physica Scripta, vol. 2005, no. T121, pp. 57–64, 2005. View at Publisher · View at Google Scholar
  17. K. Kimura, A. Takamura, and H. Yokomakura, “Exact formulas and simple dependence of neutrino oscillation probabilities in matter with constant density,” Physical Review D, vol. 66, Article ID 073005, p. 073005, 2002. View at Publisher · View at Google Scholar
  18. H. W. Zaglauer and K. H. Schwarzer, “The mixing angles in matter for three generations of neutrinos and the MSW mechanism,” Zeitschrift für Physik C: Particles and Fields, vol. 40, no. 2, pp. 273–282, 1988. View at Publisher · View at Google Scholar · View at Scopus
  19. K. Kimura, A. Takamura, and H. Yokomakura, “Exact formula of probability and CP violation for neutrino oscillations in matter,” Physics Letters B, vol. 537, pp. 86–94, 2002. View at Publisher · View at Google Scholar
  20. J. Arafune, M. Koike, and J. Sato, “CP violation and matter effect in long baseline neutrino oscillation experiments,” Physical Review D, vol. 56, p. 3093, 1997. View at Publisher · View at Google Scholar
  21. M. Freund, “Analytic approximations for three neutrino oscillation parameters and probabilities in matter,” Physical Review D, vol. 64, Article ID 053003, 2001. View at Publisher · View at Google Scholar
  22. O. Peres and A. Y. Smirnov, “Atmospheric neutrinos: LMA oscillations, Ue3 induced interference and CP-violation,” Nuclear Physics B, vol. 680, Article ID 0309312, pp. 479–509, 2004. View at Publisher · View at Google Scholar
  23. E. K. Akhmedov, R. Johansson, M. Lindner, T. Ohls-son, and T. Schwetz, “Series expansions for three-flavor neutrino oscillation probabilities in matter,” Journal of High Energy Physics, vol. 2004, article 078, 2004. View at Publisher · View at Google Scholar
  24. E. K. Akhmedov, M. Tortola, and J. Valle, “A simple analytic three-flavour description of the day-night effect in the solar neutrino flux,” Journal of High Energy Physics, vol. 2004, no. 5, article 057, 2004. View at Publisher · View at Google Scholar
  25. E. K. Akhmedov and V. Niro, “An accurate analytic description of neutrino oscillations in matter,” Journal of High Energy Physics, vol. 2008, no. 12, article 106, 2008. View at Google Scholar
  26. A. Cervera, A. Donini, M. Gavela et al., “Golden measurements at a neutrino factory,” Nuclear Physics B, vol. 579, no. 1-2, pp. 17–55, 2000. View at Publisher · View at Google Scholar
  27. D. A. Dwyer, “The improved measurement of electron-antineutrino disappearance at daya bay,” http://arxiv.org/abs/1303.3863.
  28. K. Hagiwara, N. Okamura, and K.-I. Senda, “The earth matter effects in neutrino oscillation experiments from Tokai to Kamioka and Korea,” Journal of High Energy Physics, vol. 82, 2011. View at Publisher · View at Google Scholar
  29. J. Beringer, J.-F. Arguin, R. M. Barnett et al., “Review of particle physics,” Physical Review D, vol. 86, no. 1, Article ID 010001, 2012. View at Publisher · View at Google Scholar
  30. J. D. Hunter, “Matplotlib: a 2D graphics environment,” Computing in Science & Engineering, vol. 9, pp. 90–95, 2007. View at Google Scholar