Theory of surface second-harmonic generation for semiconductors including effects of nonlocal operators

被引:19
作者
Anderson, Sean M. [1 ]
Tancogne-Dejean, Nicolas [2 ,3 ]
Mendoza, Bernardo S. [1 ]
Veniard, Valerie [2 ,3 ]
机构
[1] Ctr Invest Opt, Guanajuato, Mexico
[2] CEA DSM, CNRS, Ecole Polytech, Solides Irradies Lab, F-91128 Palaiseau, France
[3] ETSF, Palaiseau, France
关键词
NONLINEAR-OPTICAL SPECTROSCOPY; SUM-FREQUENCY GENERATION; BULK CONTRIBUTION; SILICON SURFACES; BAND THEORY; INTERFACES; ENERGY; SI(001); SUSCEPTIBILITIES; PSEUDOPOTENTIALS;
D O I
10.1103/PhysRevB.91.075302
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We formulate a theoretical approach of surface second-harmonic generation from semiconductor surfaces based on the length gauge and the electron density operator. Within the independent particle approximation, the nonlinear second-order surface susceptibility tensor chi(abc)(-2 omega; omega,omega) is calculated, including in one unique formulation (i) the scissors correction, needed to have the correct value of the energy band gap, (ii) the contribution of the nonlocal part of the pseudopotentials, routinely used in ab initio band-structure calculations, and (iii) the derivation for the inclusion of the cut function, used to extract the surface response. The first two contributions are described by spatially nonlocal quantum-mechanical operators and are fully taken into account in the present formulation. As a test case of the approach, we calculate chi(xxx) (-2 omega; omega,omega) for the clean Si(001) 2 x 1 reconstructed surface. The effects of the scissors correction and of the nonlocal part of the pseudopotentials are discussed in surface nonlinear optics. The scissors correction shifts the spectrum to higher energies though the shifting is not rigid and mixes the 1 omega and 2 omega resonances, and has a strong influence in the line shape. The effects of the nonlocal part of the pseudopotentials keeps the same line shape of vertical bar chi(xxx)(2x1)(-2 omega; omega,omega)vertical bar, but reduces its value by 15%-20%. Therefore the inclusion of the three aforementioned contributions is very important and makes our scheme unprecedented and opens the possibility to study surface second-harmonic generation with more versatility and providing more accurate results.
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页数:12
相关论文
共 72 条
[1]   THE CRYSTAL MOMENTUM AS A QUANTUM MECHANICAL OPERATOR [J].
ADAMS, EN .
JOURNAL OF CHEMICAL PHYSICS, 1953, 21 (11) :2013-2017
[2]   Nonlocality and many-body effects in the optical properties of semiconductors [J].
Adolph, B ;
Gavrilenko, VI ;
Tenelsen, K ;
Bechstedt, F ;
DelSole, R .
PHYSICAL REVIEW B, 1996, 53 (15) :9797-9808
[3]   Influence of crystal structure and quasiparticle effects on second-harmonic generation: Silicon carbide polytypes [J].
Adolph, B ;
Bechstedt, F .
PHYSICAL REVIEW B, 2000, 62 (03) :1706-1712
[4]   Microscopic study of surface second-harmonic generation from a clean Si(100) c(4X2) surface -: art. no. 125303 [J].
Arzate, N ;
Mendoza, BS .
PHYSICAL REVIEW B, 2001, 63 (12)
[5]   Screened-exchange LDA methods for films and superlattices with applications to the Si(100)2X1 surface and InAs/InSb superlattices [J].
Asahi, R ;
Mannstadt, W ;
Freeman, AJ .
PHYSICAL REVIEW B, 2000, 62 (04) :2552-2561
[6]   ENERGY-BAND THEORY OF SECOND-ORDER NONLINEAR OPTICAL SUSCEPTIBILITY OF CRYSTALS OF ZINCBLENDE SYMMETRY [J].
ASPNES, DE .
PHYSICAL REVIEW B, 1972, 6 (12) :4648-4659
[7]   Nonlinear optics from an ab initio approach by means of the dynamical Berry phase: Application to second- and third-harmonic generation in semiconductors [J].
Attaccalite, C. ;
Gruening, M. .
PHYSICAL REVIEW B, 2013, 88 (23)
[8]   NONLINEAR-OPTICAL SUSCEPTIBILITIES OF SEMICONDUCTORS - RESULTS WITH A LENGTH-GAUGE ANALYSIS [J].
AVERSA, C ;
SIPE, JE .
PHYSICAL REVIEW B, 1995, 52 (20) :14636-14645
[9]   Surface nonlinear optics: a historical overview [J].
Bloembergen, N .
APPLIED PHYSICS B-LASERS AND OPTICS, 1999, 68 (03) :289-293
[10]  
BLOUNT EI, 1962, SOLID STATE PHYS, V13, P305