发明名称 |
Wavelength conversion device and image display device |
摘要 |
The present application discloses a wavelength conversion device. The wavelength conversion device includes a light source for generating excitation light, a laser medium for generating fundamental light from the excitation light, a resonator mirror for forming a resonator for the fundamental light in cooperation with the laser medium, and a wavelength convertor for converting wavelength from the fundamental light into harmonic light. The wavelength convertor includes a first end surface inclined by an angle θ from a surface orthogonal to an optical axis of the resonator and a second end surface parallel to the first end surface. |
申请公布号 |
US9048611(B2) |
申请公布日期 |
2015.06.02 |
申请号 |
US201214000499 |
申请日期 |
2012.04.02 |
申请人 |
PANASONIC INTELLECTUAL PROPERTY MANAGEMENT CO., LTD. |
发明人 |
Nakayama Kenji;Mizushima Tetsuro;Itoh Tatsuo;Oowaki Hirohiko;Matsuo Tomohiro |
分类号 |
G02F1/35;H01S3/10;H01S3/08;H01S3/00;H01S3/109;G03B21/20;H01S3/02;H01S3/06;H01S3/23;H01S3/16 |
主分类号 |
G02F1/35 |
代理机构 |
Wenderoth, Lind & Ponack L.L.P. |
代理人 |
Wenderoth, Lind & Ponack L.L.P. |
主权项 |
1. A wavelength conversion device comprising:
a light source configured to generate excitation light; a laser medium configured to generate fundamental light from the excitation light; a resonator mirror configured to form a resonator for the fundamental light in cooperation with the laser medium; and a wavelength convertor configured to convert wavelength from the fundamental light into harmonic light, wherein the wavelength convertor includes a first end surface inclined by an angle θ from a surface orthogonal to an optical axis of the resonator and a second end surface parallel to the first end surface, and the angle θ satisfies a relationship represented by Formulas 1 to 5 described below:SpreadingAngleofHarmonicLight<θ<θ1=12tan-1(ϕ1+ϕ22L1)[Formula1] where, L1: length of the laser medium in an optical axis direction, and φ1 and φ2 are defined by Formula 2:ϕ1=2(λ2π)4L(R-L)ϕ2=ϕ11+2(L1)2(πn0ϕ124λ)2[Formula2] where, λ: wavelength of the fundamental light, L: resonator length, π: circular constant, R: curvature radius of the resonator mirror, and n0 is defined by Formula 3:n0=n′L′[Formula3]where n′ is defined by Formula 4 and L′ is defined by Formula 5:n′=n1L1+n2(L2-L1)+L2-L1cos2θ+L1cos{sin-1(n1n2sin2θ)}[Formula4] where, n1: refractive index of the laser medium, n2: refractive index between the laser medium and the wavelength convertor, L2: distance from the laser medium to the wavelength convertor,L′=L2+L2-L1cos2θ+L1cos{sin-1(n1n2sin2θ)}.[Formula5] |
地址 |
Osaka JP |