erratum to: quantum well intermixed waveguide grating

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Opt Quant Electron (2012) 44:373 DOI 10.1007/s11082-012-9547-2 ERRATUM Erratum to: Quantum well intermixed waveguide grating Ramesh K. Sonkar · Utpal Das Published online: 28 January 2012 © Springer Science+Business Media, LLC. 2012 Erratum to: Opt Quant Electron (2011) 42:631–643 DOI 10.1007/s11082-011-9486-3 The authors would like to correct the incorrect text and equations in the original publication of the article. Paragraph 1 in the published article (in page 637) should read as “Band to band transi- tion as well as excitonic effects was taken into consideration while calculating the dielectric constants.” The correct version of the Eqs. 12 and 13 is given in detail below ε QW 2 (ω) = C ω 2 mn m hh O h mn 2 ¯ hω E hh mn + m lh 3 O l mn 2 ¯ hω E lh imn (12) where O h mn and O l mn are the overlap integrals of m th conduction band eigen function and n th VB eigen function for HH and LH, respectively. With C = π e 2 P 2 CV / ¯ h 2 m 0 W ε 0 . where, P 2 CV = (2/ m 0 )s | p x |x 2 is a parameter related to the squared matrix element. m hh and m lh are the reduced electron-heavy hole and electron-light hole masses respectively. ε 1 (ω) = 1 + ε b + C πω 2 mn m hh O h mn 2 ln ( E hh mn ) 2 ( E hh mn ) 2 ( ¯ hω) 2 + m lh 3 O l mn 2 ln ( E lh mn ) 2 ( E lh mn ) 2 ( ¯ hω) 2 (13) The online version of the original article can be found under doi:10.1007/s11082-011-9486-3. R. K. Sonkar (B ) · U. Das Department of Electrical Engineering, Indian Institute of Technology, Kanpur, India e-mail: [email protected] 123

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Page 1: Erratum to: Quantum well intermixed waveguide grating

Opt Quant Electron (2012) 44:373DOI 10.1007/s11082-012-9547-2

ERRATUM

Erratum to: Quantum well intermixed waveguide grating

Ramesh K. Sonkar · Utpal Das

Published online: 28 January 2012© Springer Science+Business Media, LLC. 2012

Erratum to: Opt Quant Electron (2011) 42:631–643DOI 10.1007/s11082-011-9486-3

The authors would like to correct the incorrect text and equations in the original publicationof the article.

Paragraph 1 in the published article (in page 637) should read as “Band to band transi-tion as well as excitonic effects was taken into consideration while calculating the dielectricconstants.”

The correct version of the Eqs. 12 and 13 is given in detail below

εQW2 (ω) = C

ω2

mn

[mhh

∣∣∣Ohmn

∣∣∣2�

(h̄ω − Ehh

mn

)+ mlh

3

∣∣∣Olmn

∣∣∣2�

(h̄ω − Elh

imn

)](12)

where Ohmn and Ol

mn are the overlap integrals of mth conduction band eigen function andnth VB eigen function for HH and LH, respectively. With C = πe2 P2

CV /h̄2m0Wε0. where,P2

CV = (2/m0)〈s|px |x〉2 is a parameter related to the squared matrix element. mhh and mlh

are the reduced electron-heavy hole and electron-light hole masses respectively.

ε1 (ω) = 1 + εb + C

πω2

mn

[mhh

∣∣∣Ohmn

∣∣∣2

ln

∣∣∣∣∣

(Ehh

mn

)2

(Ehh

mn

)2 − (h̄ω)2

∣∣∣∣∣

+mlh

3

∣∣∣Olmn

∣∣∣2

ln

∣∣∣∣∣

(Elh

mn

)2

(Elh

mn

)2 − (h̄ω)2

∣∣∣∣∣

](13)

The online version of the original article can be found under doi:10.1007/s11082-011-9486-3.

R. K. Sonkar (B) · U. DasDepartment of Electrical Engineering, Indian Institute of Technology, Kanpur, Indiae-mail: [email protected]

123