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Table 1 Lattice parameters, energy gaps, our calculated ε 1 ⊥ ( 0 ) MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaciaacaqabeaabeqacmaaaOqaaiabew7aLnaaDaaaleaacqaIXaqmaeaacqGHLkIxaaGcdaqadaqaaiabicdaWaGaayjkaiaawMcaaaaa@31ED@ and ε 2 I I ( 0 ) MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaciaacaqabeaabeqacmaaaOqaaiabew7aLnaaDaaaleaacqaIYaGmaeaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaeHbbjxAHXgaiqaacaWFjbGaa8xsaaaakmaabmaabaGaeGimaadacaGLOaGaayzkaaaaaa@3B85@ and Δn(0).

From: Electronic structure, linear, nonlinear optical susceptibilities and birefringence of CuInX2(X = S, Se, Te) chalcopyrite-structure compounds

 

CuInS2

CuInSe2

CuInTe2

A (Ã…)

5.52a

5.78a

6.179a

C (Ã…)

11.08a

11.57a

12.36a

E g exp . MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaciaacaqabeaabeqacmaaaOqaaiabdweafnaaDaaaleaacqWGNbWzaeaacyGGLbqzcqGG4baEcqGGWbaCcqGGUaGlaaaaaa@32A6@ (eV)

1.53b, r, 1.55e, 1.48i, 1.54d

1.04b, 0.96g, 1.01h, 0.98i, r, 0.88d

1.06b, j, 0.96f

E g T h e o r y MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaciaacaqabeaabeqacmaaaOqaaiabdweafnaaDaaaleaacqWGNbWzaeaacqWGubavcqWGObaAcqWGLbqzcqWGVbWBcqWGYbGCcqWG5bqEaaaaaa@35BA@ (eV)

0.01c, -0.14r, 0.812*

0.01c, -0.2r, 0.416*

0.18c, 0.424*

ε 1 ⊥ ( 0 ) MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaciaacaqabeaabeqacmaaaOqaaiabew7aLnaaDaaaleaacqaIXaqmaeaacqGHLkIxaaGcdaqadaqaaiabicdaWaGaayjkaiaawMcaaaaa@31ED@

11.3*, 9.71p, 8.6q

14.8*

13.5*

ε 1 I I ( 0 ) MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8bkY=wiFfYlOipiY=Hhbbf9v8qqaqFr0xc9vqpe0di9q8qqpG0dHiVcFbIOFHK8Feei0lXdar=Jb9qqFfeaYRXxe9vr0=vr0=LqpWqaaeaabiGaciaacaqabeaabeqacmaaaOqaaiabew7aLnaaDaaaleaacqaIXaqmaeaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaeHbbjxAHXgaiqaacaWFjbGaa8xsaaaakmaabmaabaGaeGimaadacaGLOaGaayzkaaaaaa@3B83@

11*, 9.68p, 8.4q

14.6*

13.8*

Δn(0)

-0.018k, -0.019*

-0.012m, -0.013*

0.002*

N 0

2.532n, o, 2.71*

2.606n, 2.83*

2.720n, 2.91*

  1. aRef.32 bRef.36 cRef.17 dRef.37 eRef.38 fRef. 11 gRef.39 hRef.40 iRef.41 jRef.42 kRef.19 mRef.20 nRef.31 oRef.57 pRef.53 qRef.62 rRef.63
  2. *This work