LEADER 04462nam 22007455 450 001 9910845083303321 005 20240321185758.0 010 $a981-9706-18-1 024 7 $a10.1007/978-981-97-0618-1 035 $a(MiAaPQ)EBC31214004 035 $a(Au-PeEL)EBL31214004 035 $a(MiAaPQ)EBC31222670 035 $a(Au-PeEL)EBL31222670 035 $a(DE-He213)978-981-97-0618-1 035 $a(CKB)30927949600041 035 $a(EXLCZ)9930927949600041 100 $a20240316d2024 u| 0 101 0 $aeng 135 $aurcnu|||||||| 181 $ctxt$2rdacontent 182 $cc$2rdamedia 183 $acr$2rdacarrier 200 10$aSecond-Order Photogalvanic Photocurrents in 2D Materials$b[electronic resource] /$fby Mustafa Eginligil, Ting Yu 205 $a1st ed. 2024. 210 1$aSingapore :$cSpringer Nature Singapore :$cImprint: Springer,$d2024. 215 $a1 online resource (129 pages) 225 1 $aNanoscience and Nanotechnology,$x2196-1689 311 $a981-9706-17-3 327 $a1. Introduction to light polarization-dependent photocurrent ? phenomenology -- 2. Graphene as the model low-dimensional photogalvanic material -- 3. Light helicity dependent photocurrent in graphene planes -- 4. Influence of spin-valley coupling on photogalvanic photocurrents in layered transition metal dichalcogenides -- 5. Light helicity dependent photocurrent in layered transition metal dichalcogenides. 330 $aThis book highlights the photogalvanic effects at low dimensions, surfaces, and interfaces, more specifically 2D materials, such as graphene and monolayer transition metal dichalcogenides. Although the phenomenology of the photogalvanic effects, which can be simply seen as photoresponse nonlinear-in-electric field, have been well-established, the microscopic understanding in each material system may vary. This book is a quick reference and a detailed roadmap starting from phenomenology and continuing with the ultimate low dimensional materials, in which the photogalvanic effects can offer a rich platform at the second-order response to an electric field. A general phenomenology of photogalvanic effect is provided in the first chapter, together with the photon drag effect which also generates a photocurrent like the photogalvanic effect, but with some distinct features, as well as somewhat puzzling similarities. Next two chapters explain these effects in graphene, starting with a necessary related background on graphene, then a particular focus on its specific phenomenology, microscopic theory, and experimental results. In a similar fashion, in chapters four and five, a necessary background for the photogalvanic effects in monolayer transition metal dichalcogenides, with symmetry analysis, microscopic theory, and experimental results is presented, along with the Berry curvature dependent photocurrent, which can also play an important role in 2D semiconductors. The second-order photogalvanic effects that have been covered so far in graphene and monolayer transition metal chalcogenides have already excited the 2D semiconductor optoelectronic research community by several means. It seems that the interests on the photogalvanic effects will continue to escalate in near future. 410 0$aNanoscience and Nanotechnology,$x2196-1689 606 $aOptical materials 606 $aTelecommunication 606 $aLasers 606 $aNanochemistry 606 $aSolid state physics 606 $aNanotechnology 606 $aOptical Materials 606 $aMicrowaves, RF Engineering and Optical Communications 606 $aLaser 606 $aNanochemistry 606 $aElectronic Devices 606 $aNanotechnology 615 0$aOptical materials. 615 0$aTelecommunication. 615 0$aLasers. 615 0$aNanochemistry. 615 0$aSolid state physics. 615 0$aNanotechnology. 615 14$aOptical Materials. 615 24$aMicrowaves, RF Engineering and Optical Communications. 615 24$aLaser. 615 24$aNanochemistry. 615 24$aElectronic Devices. 615 24$aNanotechnology. 676 $a620.11295 700 $aEginligil$b Mustafa$01733714 701 $aYu$b Ting$0874886 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910845083303321 996 $aSecond-Order Photogalvanic Photocurrents in 2D Materials$94149604 997 $aUNINA