Yalin Lu

Hiroshi Murata

Chang-Qing Xu

Progress in Domain-Engineered Photonics Materials

the detect optic signal modul 15 ghz demonstr experiment use differ frequenc generat base secondord nonlinear optic effect period pole microwav rectangular waveguid the measur frequenc depend generat microwav signal good agreement theoret expect result interest applic propos devic detect highspe optic clock detect

Yasuyuki Okamura

Detection of an Optical Signal Using Difference Frequency Generation in a Periodically Poled <svg style="vertical-align:-4.49648pt;width:65.150002px;" id="M1" height="20.85" version="1.1" viewBox="0 0 65.150002 20.85" width="65.150002" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg"><g transform="matrix(.022,-0,0,-.022,.062,15.188)"><path id="x4C" d="M495 163l30 -6q-19 -99 -36 -157h-453v28q63 5 77.5 20t14.5 78v400q0 63 -13 77t-75 19v28h261v-28q-61 -5 -74.5 -19t-13.5 -77v-395q0 -41 5 -59t18 -25q24 -13 96 -13q85 0 112 31q30 33 51 98z" /></g><g transform="matrix(.022,-0,0,-.022,12.235,15.188)"><path id="x69" d="M135 536q-20 0 -35 15.5t-15 35.5q0 22 15 37t36 15t35.5 -15t14.5 -37q0 -21 -15 -36t-36 -15zM252 0h-220v26q48 5 59 17t11 63v206q0 47 -9 58t-54 18v24q78 12 142 39v-345q0 -51 11.5 -63t59.5 -17v-26z" /></g><g transform="matrix(.022,-0,0,-.022,18.242,15.188)"><path id="x54" d="M592 498l-30 -3q-13 63 -31 89q-13 19 -33.5 25.5t-75.5 6.5h-70v-493q0 -60 16 -75.5t86 -19.5v-28h-286v28q68 4 83.5 19.5t15.5 75.5v493h-62q-60 0 -83 -7t-33 -24q-12 -17 -32 -90h-29q10 116 12 180h20q10 -16 21 -20.5t34 -4.5h395q19 0 28.5 5t21.5 20h21&#xA;q2 -89 11 -177z" /></g><g transform="matrix(.022,-0,0,-.022,30.033,15.188)"><path id="x61" d="M433 39l-85 -51q-27 0 -47 20q-16 16 -24 44q-5 -3 -24 -16.5t-27 -18.5t-23 -13.5t-25 -12t-19 -3.5q-52 0 -86 36.5t-34 85.5q0 71 81 99q128 43 155 65v17q0 54 -23 83.5t-62 29.5q-28 0 -45 -19t-29 -66q-7 -23 -29 -23q-15 0 -29 13t-14 30t31 40q25 19 68.5 40.5&#xA;t81.5 29.5q49 0 82 -27q45 -39 45 -123v-185q0 -60 35 -60q18 0 36 11zM275 84v156q-12 -6 -49 -23t-41 -19q-31 -14 -46 -31t-15 -43q0 -35 22.5 -55.5t48.5 -20.5q19 0 42 10.5t38 25.5z" /></g><g transform="matrix(.022,-0,0,-.022,39.874,15.188)"><path id="x4F" d="M381 665q131 0 226.5 -93t95.5 -239q0 -158 -96 -253t-238 -95q-137 0 -231 95t-94 238q0 142 92.5 244.5t244.5 102.5zM359 629q-89 0 -151 -74.5t-62 -208.5q0 -141 69 -233t175 -92q90 0 150.5 74t60.5 211q0 152 -69 237.5t-173 85.5z" /></g><g transform="matrix(.016,-0,0,-.016,56.612,20.575)"><path id="x1D7D1" d="M58 524l-21 12q80 152 229 152q73 0 119 -41q45 -41 45 -96q0 -40 -21.5 -74.5t-62.5 -52.5q57 -20 89.5 -68.5t32.5 -109.5q0 -110 -86 -185t-214 -75q-69 0 -110.5 24.5t-41.5 65.5q0 26 18.5 43t46.5 17q45 0 96 -57q39 -43 79 -43q45 0 71.5 34t26.5 88q0 75 -49 121&#xA;q-25 23 -56 39q-34 17 -97 38v17q69 21 100 53t31 78q0 103 -99 103q-40 0 -69.5 -19t-56.5 -64z" /></g></svg> Microwave Waveguide

optical waveguid were fabric zcut stoichiometr slt use protonexchang method the surfac index chang extraordinari ray slt substrat result from proton exchang 0017 which coincid well congruent substrat the proton exchang coeffici slt the applic slt waveguid quasivelocitymatch travellingwav electroopt modul period polarizationrevers structur also report

Fabrication of Proton-Exchange Waveguide Using  Stoichiometric <svg style="vertical-align:-4.47125pt;width:64.837502px;" id="M1" height="20.825001" version="1.1" viewBox="0 0 64.837502 20.825001" width="64.837502" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg"><g transform="matrix(.022,-0,0,-.022,.062,15.188)"><path id="x4C" d="M495 163l30 -6q-19 -99 -36 -157h-453v28q63 5 77.5 20t14.5 78v400q0 63 -13 77t-75 19v28h261v-28q-61 -5 -74.5 -19t-13.5 -77v-395q0 -41 5 -59t18 -25q24 -13 96 -13q85 0 112 31q30 33 51 98z" /></g><g transform="matrix(.022,-0,0,-.022,12.235,15.188)"><path id="x69" d="M135 536q-20 0 -35 15.5t-15 35.5q0 22 15 37t36 15t35.5 -15t14.5 -37q0 -21 -15 -36t-36 -15zM252 0h-220v26q48 5 59 17t11 63v206q0 47 -9 58t-54 18v24q78 12 142 39v-345q0 -51 11.5 -63t59.5 -17v-26z" /></g><g transform="matrix(.022,-0,0,-.022,18.242,15.188)"><path id="x54" d="M592 498l-30 -3q-13 63 -31 89q-13 19 -33.5 25.5t-75.5 6.5h-70v-493q0 -60 16 -75.5t86 -19.5v-28h-286v28q68 4 83.5 19.5t15.5 75.5v493h-62q-60 0 -83 -7t-33 -24q-12 -17 -32 -90h-29q10 116 12 180h20q10 -16 21 -20.5t34 -4.5h395q19 0 28.5 5t21.5 20h21&#xA;q2 -89 11 -177z" /></g><g transform="matrix(.022,-0,0,-.022,30.033,15.188)"><path id="x61" d="M433 39l-85 -51q-27 0 -47 20q-16 16 -24 44q-5 -3 -24 -16.5t-27 -18.5t-23 -13.5t-25 -12t-19 -3.5q-52 0 -86 36.5t-34 85.5q0 71 81 99q128 43 155 65v17q0 54 -23 83.5t-62 29.5q-28 0 -45 -19t-29 -66q-7 -23 -29 -23q-15 0 -29 13t-14 30t31 40q25 19 68.5 40.5&#xA;t81.5 29.5q49 0 82 -27q45 -39 45 -123v-185q0 -60 35 -60q18 0 36 11zM275 84v156q-12 -6 -49 -23t-41 -19q-31 -14 -46 -31t-15 -43q0 -35 22.5 -55.5t48.5 -20.5q19 0 42 10.5t38 25.5z" /></g><g transform="matrix(.022,-0,0,-.022,39.874,15.188)"><path id="x4F" d="M381 665q131 0 226.5 -93t95.5 -239q0 -158 -96 -253t-238 -95q-137 0 -231 95t-94 238q0 142 92.5 244.5t244.5 102.5zM359 629q-89 0 -151 -74.5t-62 -208.5q0 -141 69 -233t175 -92q90 0 150.5 74t60.5 211q0 152 -69 237.5t-173 85.5z" /></g><g transform="matrix(.016,-0,0,-.016,56.612,20.575)"><path id="x33" d="M285 378v-2q65 -13 102 -54.5t37 -97.5q0 -57 -30.5 -104.5t-74 -75t-85.5 -42t-72 -14.5q-31 0 -59.5 11t-40.5 23q-19 18 -16 36q1 16 23 33q13 10 24 0q58 -51 124 -51q55 0 88 40t33 112q0 64 -39 96.5t-88 32.5q-29 0 -64 -11l-6 29q77 25 118 57.5t41 84.5&#xA;q0 45 -26.5 69.5t-68.5 24.5q-67 0 -120 -79l-20 20l43 63q51 56 127 56h1q66 0 107 -37t41 -95q0 -42 -31 -71q-22 -23 -68 -54z" /></g></svg> for Guided Wave Electrooptic  Modulators with Polarization-Reversed Structure

nois characterist secondharmon generat shg period pole lithium niobat ppln use quasiphas match qpm techniqu analyz experiment experi a078 secondharmon wave generat when 156 fundament wave pass through ppln crystal bulk waveguid the timedomain frequencydomain nois characterist fundament wave were analyz use pumpprob method nois characterist shg were further analyz when visibl light 532 infrar light 1090 copropag fundament light respect the nois character were also investig differ temperatur found bulk waveguid ppln crystal wave has higher relat nois level than correspond fundament wave for same fundament wave wave has lower nois bulk crystal than waveguid mgodope ppln than undop ppln the 532 irradi can lead higher nois ppln than 1090 irradi addit increas temperatur devic can allevi problem nois conjunct photorefract effect incur irradi light this more signific undop ppln than mgodope one

Yong Wang

Jorge Fonseca-Campos

Wan-guo Liang

Ignacio Vargas-Baca

Noise Analysis of Second-Harmonic Generation in Undoped and MgO-Doped Periodically Poled Lithium Niobate

estim phase veloc modul microwav quasivelocitymatch qvm electroopt phase modul qvmeom use sampl which accur most reliabl techniqu measur voltag waveform electrod the substrat measur qvmeom stoichiometr period domaininvert crystal the electr field stand wave reson microstrip line width 05 height 05 measur employ cdte crystal sensor the wavelength travel microwav 160801 ghz determin 333 fit theoret curv measur electr field distribut the phase veloc estim though exist about 5 systemat error due perturb sensor relat dielectr constant led maximum likelihood valu deriv estim phase veloc

Shintaro Hisatake

Akira Kaino

Tomoaki Yasuda

Tadao Nagatsuma

Phase Velocity Estimation of a Microstrip Line in  a Stoichiometric Periodically Domain-Inverted 
<svg style="vertical-align:-4.47125pt;width:64.837502px;" id="M1" height="20.825001" version="1.1" viewBox="0 0 64.837502 20.825001" width="64.837502" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg"><g transform="matrix(.022,-0,0,-.022,.062,15.188)"><path id="x4C" d="M495 163l30 -6q-19 -99 -36 -157h-453v28q63 5 77.5 20t14.5 78v400q0 63 -13 77t-75 19v28h261v-28q-61 -5 -74.5 -19t-13.5 -77v-395q0 -41 5 -59t18 -25q24 -13 96 -13q85 0 112 31q30 33 51 98z" /></g><g transform="matrix(.022,-0,0,-.022,12.235,15.188)"><path id="x69" d="M135 536q-20 0 -35 15.5t-15 35.5q0 22 15 37t36 15t35.5 -15t14.5 -37q0 -21 -15 -36t-36 -15zM252 0h-220v26q48 5 59 17t11 63v206q0 47 -9 58t-54 18v24q78 12 142 39v-345q0 -51 11.5 -63t59.5 -17v-26z" /></g><g transform="matrix(.022,-0,0,-.022,18.242,15.188)"><path id="x54" d="M592 498l-30 -3q-13 63 -31 89q-13 19 -33.5 25.5t-75.5 6.5h-70v-493q0 -60 16 -75.5t86 -19.5v-28h-286v28q68 4 83.5 19.5t15.5 75.5v493h-62q-60 0 -83 -7t-33 -24q-12 -17 -32 -90h-29q10 116 12 180h20q10 -16 21 -20.5t34 -4.5h395q19 0 28.5 5t21.5 20h21&#xA;q2 -89 11 -177z" /></g><g transform="matrix(.022,-0,0,-.022,30.033,15.188)"><path id="x61" d="M433 39l-85 -51q-27 0 -47 20q-16 16 -24 44q-5 -3 -24 -16.5t-27 -18.5t-23 -13.5t-25 -12t-19 -3.5q-52 0 -86 36.5t-34 85.5q0 71 81 99q128 43 155 65v17q0 54 -23 83.5t-62 29.5q-28 0 -45 -19t-29 -66q-7 -23 -29 -23q-15 0 -29 13t-14 30t31 40q25 19 68.5 40.5&#xA;t81.5 29.5q49 0 82 -27q45 -39 45 -123v-185q0 -60 35 -60q18 0 36 11zM275 84v156q-12 -6 -49 -23t-41 -19q-31 -14 -46 -31t-15 -43q0 -35 22.5 -55.5t48.5 -20.5q19 0 42 10.5t38 25.5z" /></g><g transform="matrix(.022,-0,0,-.022,39.874,15.188)"><path id="x4F" d="M381 665q131 0 226.5 -93t95.5 -239q0 -158 -96 -253t-238 -95q-137 0 -231 95t-94 238q0 142 92.5 244.5t244.5 102.5zM359 629q-89 0 -151 -74.5t-62 -208.5q0 -141 69 -233t175 -92q90 0 150.5 74t60.5 211q0 152 -69 237.5t-173 85.5z" /></g><g transform="matrix(.016,-0,0,-.016,56.612,20.575)"><path id="x33" d="M285 378v-2q65 -13 102 -54.5t37 -97.5q0 -57 -30.5 -104.5t-74 -75t-85.5 -42t-72 -14.5q-31 0 -59.5 11t-40.5 23q-19 18 -16 36q1 16 23 33q13 10 24 0q58 -51 124 -51q55 0 88 40t33 112q0 64 -39 96.5t-88 32.5q-29 0 -64 -11l-6 29q77 25 118 57.5t41 84.5&#xA;q0 45 -26.5 69.5t-68.5 24.5q-67 0 -120 -79l-20 20l43 63q51 56 127 56h1q66 0 107 -37t41 -95q0 -42 -31 -71q-22 -23 -68 -54z" /></g></svg>  Modulator Using Electro-Optic Sampling Technique

nonlinear frequenc convers remain one domin approach effici generat thz wave signific materi absorpt thz rang main factor imped progress toward direct research new multiclad nonlinear fiber design propos solv problem major experiment effort period domain structur introduc lithium niobat singlecryst fiber electr pole the introduc period domain structur were nondestruct reveal use crossli polar optic microscop confoc scan optic microscop qualiti assur

Kitt Reinhardt

Domain-Reversed Lithium Niobate Single-Crystal Fibers are Potentially for Efficient Terahertz Wave Generation

908 green light 532 were generat intracav quasiphas match bulk period pole mgo ppmgln crystal maximum opticaltoopt convers effici 335 obtain from 05 thick 10 long 5 mol mgo crystal endpump power 27 808 the temperatur bandwidth between intracav singlepass frequenc doubl found differ ppmgln reliabl stabil green laser were evalu found continu oper 100 hour output stabil better than 975 optic damag observ

Shaowei Chu

Ying Zhang

Bin Wang

Yong Bi

High-Efficiency Intracavity Continuous-Wave  Green-Light Generation by Quasiphase Matching in  a Bulk Periodically Poled MgO:<svg     style="vertical-align:-4.47125pt;width:71.337502px;" id="M1" height="21.65" version="1.1" viewBox="0 0 71.337502 21.65" width="71.337502"  xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg">
	
		
			<g transform="matrix(.022,-0,0,-.022,.062,16.025)"><path id="x4C" d="M495 163l30 -6q-19 -99 -36 -157h-453v28q63 5 77.5 20t14.5 78v400q0 63 -13 77t-75 19v28h261v-28q-61 -5 -74.5 -19t-13.5 -77v-395q0 -41 5 -59t18 -25q24 -13 96 -13q85 0 112 31q30 33 51 98z" /></g><g transform="matrix(.022,-0,0,-.022,12.235,16.025)"><path id="x69" d="M135 536q-20 0 -35 15.5t-15 35.5q0 22 15 37t36 15t35.5 -15t14.5 -37q0 -21 -15 -36t-36 -15zM252 0h-220v26q48 5 59 17t11 63v206q0 47 -9 58t-54 18v24q78 12 142 39v-345q0 -51 11.5 -63t59.5 -17v-26z" /></g><g transform="matrix(.022,-0,0,-.022,18.242,16.025)"><path id="x4E" d="M719 650v-28q-43 -2 -62 -15t-22 -44q-6 -47 -6 -169v-403h-31l-426 524h-2v-251q0 -111 6 -169q4 -37 24 -50.5t72 -16.5v-28h-237v28q45 2 64.5 16t23.5 49q6 62 6 171v220q0 54 -3 68.5t-17 32.5q-16 19 -34.5 26.5t-54.5 10.5v28h147l418 -502h3v246q0 117 -7 166&#xA;q-4 34 -24.5 47t-73.5 15v28h236z" /></g><g transform="matrix(.022,-0,0,-.022,34.965,16.025)"><path id="x62" d="M152 404l81 35q23 10 41 10q81 0 139 -61.5t58 -149.5q0 -107 -74.5 -178.5t-176.5 -71.5q-71 0 -147 36v555q0 48 -9.5 59.5t-56.5 15.5v23q79 10 145 35v-308zM152 374v-258q0 -20 6 -35q7 -19 30 -37t58 -18q63 0 99.5 50t36.5 137q0 82 -43.5 131t-108.5 49&#xA;q-44 0 -78 -19z" /></g><g transform="matrix(.022,-0,0,-.022,46.352,16.025)"><path id="x4F" d="M381 665q131 0 226.5 -93t95.5 -239q0 -158 -96 -253t-238 -95q-137 0 -231 95t-94 238q0 142 92.5 244.5t244.5 102.5zM359 629q-89 0 -151 -74.5t-62 -208.5q0 -141 69 -233t175 -92q90 0 150.5 74t60.5 211q0 152 -69 237.5t-173 85.5z" /></g>

			<g transform="matrix(.016,-0,0,-.016,63.112,21.4)"><path id="x33" d="M285 378v-2q65 -13 102 -54.5t37 -97.5q0 -57 -30.5 -104.5t-74 -75t-85.5 -42t-72 -14.5q-31 0 -59.5 11t-40.5 23q-19 18 -16 36q1 16 23 33q13 10 24 0q58 -51 124 -51q55 0 88 40t33 112q0 64 -39 96.5t-88 32.5q-29 0 -64 -11l-6 29q77 25 118 57.5t41 84.5&#xA;q0 45 -26.5 69.5t-68.5 24.5q-67 0 -120 -79l-20 20l43 63q51 56 127 56h1q66 0 107 -37t41 -95q0 -42 -31 -71q-22 -23 -68 -54z" /></g>

		
	
</svg> Crystal

discuss new method design travelingwav electroopt modul control frequenc respons use nonperiod polarizationrevers structur using our method frequenc respons both magnitud phase modul index control sever electroopt modul advanc modul format duobinari modul wideband singlesideband modul propos

Ha Viet Pham

Electrooptic Modulators with Controlled Frequency Responses by Using Nonperiodically Polarization-Reversed Structure

have experiment demonstr effici allfib passiv qswitch ybdope fiber laser samarium dope fiber satur absorb averag output power 34 repetit rate 250 khz puls width 11 microsecond obtain pump power 90 use fiber laser system mgodope congruent period pole lithium niobat mgo cppln second harmon generat shg output 532 achiev room temperatur the convers effici around 42 which agre well theoret simul

Yi Gan

Xijia Gu

Joyce Y. C. Koo

Wanguo Liang

Chang-qing Xu

Second Harmonic Generation Using an All-Fiber Q-Switched Yb-Doped Fiber Laser and MgO:c-PPLN

oxidebas multilay structur propos realiz negat refract the multilay compos altern layer have negat permitt negat permeabl respect order realiz negat refract dielectr magnet reson layer tune frequenc close possibl via chang temperatur composit structur forth such oxidebas nims attract potenti applic optic super lens imag optic cloak sensor forth those requir lowloss lowcost good fabric flexibl

Gail J. Brown

Negative Refraction Using Frequency-Tuned Oxide Multilayer Structure

About this journal

<p>Advances in OptoElectronics publishes papers on the theory, design, fabrication, and applications of devices and components that convert light into an electrical current or, conversely, an electric current into light.</p>


Journal profile

Meet the editorial board

<p>Advances in OptoElectronics maintains an Editorial Board of practicing researchers from around the world, to ensure manuscripts are handled by editors who are experts in the field of study.</p>


Editor spotlight

Submit your proposal

Do you think there is an emerging area of research that really needs to be highlighted? Or an existing research area that has been overlooked or would benefit from deeper investigation? Raise the profile of a research area by leading a Special Issue.

Special Issues

Author guidelines

Editorial board

Databases and indexing

Advances in OptoElectronics

<p>This Issue is now open for submissions.</p>
<p>Papers are published upon acceptance, regardless of the Special Issue publication date.</p>


Advances in OptoElectronics

Progress in Domain Engineered Photonic Materials

Progress in Domain Engineered Photonic Materials

Articles

Progress in Domain-Engineered Photonics Materials

Detection of an Optical Signal Using Difference Frequency Generation in a Periodically Poled Microwave Waveguide

Fabrication of Proton-Exchange Waveguide Using Stoichiometric for Guided Wave Electrooptic Modulators with Polarization-Reversed Structure

Noise Analysis of Second-Harmonic Generation in Undoped and MgO-Doped Periodically Poled Lithium Niobate

Phase Velocity Estimation of a Microstrip Line in a Stoichiometric Periodically Domain-Inverted Modulator Using Electro-Optic Sampling Technique

Domain-Reversed Lithium Niobate Single-Crystal Fibers are Potentially for Efficient Terahertz Wave Generation

High-Efficiency Intracavity Continuous-Wave Green-Light Generation by Quasiphase Matching in a Bulk Periodically Poled MgO: Crystal

Electrooptic Modulators with Controlled Frequency Responses by Using Nonperiodically Polarization-Reversed Structure

Second Harmonic Generation Using an All-Fiber Q-Switched Yb-Doped Fiber Laser and MgO:c-PPLN

Negative Refraction Using Frequency-Tuned Oxide Multilayer Structure