Generation of optical frequency comb squeezed light field with TEM01 transverse mode

Nan Huo; Chihua Zhou; Hengxin Sun; Kui Liu; Jiangrui Gao

doi:10.3788/COL201614.062702

Journals >Chinese Optics Letters >Volume 14 >Issue 6 >Page 062702 > Article

Chinese Optics Letters
Vol. 14, Issue 6, 062702 (2016)

Generation of optical frequency comb squeezed light field with TEM₀₁ transverse mode

Nan Huo^1、2, Chihua Zhou^1、2, Hengxin Sun^1、2, Kui Liu^1、2、*, and Jiangrui Gao^1、2

Author Affiliations

¹State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan 030006, China

²Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China

show less

DOI: 10.3788/COL201614.062702 Cite this Article Set citation alerts

Nan Huo, Chihua Zhou, Hengxin Sun, Kui Liu, Jiangrui Gao. Generation of optical frequency comb squeezed light field with TEM₀₁ transverse mode[J]. Chinese Optics Letters, 2016, 14(6): 062702 Copy Citation Text

EndNote(RIS)

BibTex

Plain Text

show less

Abstract

Nonclassical optical frequency combs find tremendous utility in quantum information and high-precision quantum measurement. The characteristics of a type-I synchronously pumped optical parametric oscillator with the

{TEM}_{01}

transverse mode below threshold are investigated and a squeezing of 0.7 dB for an optical frequency comb squeezed light field with the

{TEM}_{01}

transverse mode is obtained under the pump power of 130 mW. This work has a promising application in three-dimensional space-time measurement.

{\hat{H}}_{I} = i \sum_{j, q, m} χ_{j, q, m} f_{q, m}^{j} a_{q}^{�} (t) a_{m}^{�} (t) {\hat{p}}_{j} (t) + H.c,

(1)

View in Article

χ_{j, q, m} \approx χ^{(2)} A_{I 01} = χ^{(2)} \iint u_{j} u_{m}^{*} u_{q}^{*} d x d y,

(2)

View in Article

\frac{d {\hat{a}}_{m}}{d t} = - γ {\hat{a}}_{m} - γ σ \sum_{q} f_{q, m}^{j} α_{j} {\hat{a}}_{q}^{�} + \sqrt{2 γ_{s}} {\hat{a}}_{in, m} + \sqrt{2 γ_{ν}} {\hat{a}}_{ν, m},

(3)

View in Article

\frac{d}{d t} {\hat{S}}_{m} = - γ {\hat{S}}_{m} - γ σ Λ_{m} {\hat{S}}_{m}^{�} + \sqrt{2 γ_{s}} {\hat{S}}_{in, m} + \sqrt{2 γ_{ν}} {\hat{S}}_{ν, m},

(4)

View in Article

δ^{2} {\tilde{S}}_{out, m}^{(\pm)} (ω) = \frac{γ_{s}^{2} {(1 \mp r Λ_{m} / Λ_{0})}^{2} + ω^{2}}{γ^{2} {(1 \pm r Λ_{m} / Λ_{0})}^{2} + ω^{2}},

(5)

View in Article

δ^{2} {\tilde{S}}_{out}^{(+)} (ω) = 1 - η_{total} ρ \frac{4 r}{{(1 + r)}^{2} + {(ω / γ)}^{2}},

(6)

View in Article

Nan Huo, Chihua Zhou, Hengxin Sun, Kui Liu, Jiangrui Gao. Generation of optical frequency comb squeezed light field with TEM₀₁ transverse mode[J]. Chinese Optics Letters, 2016, 14(6): 062702

Download Citation

EndNote(RIS)

BibTex

Plain Text

Set citation alerts for the article

Tools

Set citation alerts for the article

Save the article for my favorites

Paper Information