德国Layertec丨飞秒激光全反射镜 纳秒、皮秒、飞秒超快激光镜片 负色散镜 连续脉冲和纳秒激光镜片低损耗激光镜片 镀金属膜镜片 激光用滤光片 多功能带宽镜片
低损耗激光镜片 镀金属膜镜片 激光用滤光片 多功能带宽镜片
纳秒皮秒激光镜片 飞秒激光光学元件 飞秒激光反射镜 超快激光镜片及组件 负色散镜 GT干涉镜
LAYERTEC公司于1990年成立于德国，是世界的光学镜片OME厂。凭借多年在光学领域中对飞秒激光镜片的研究开发以及设计生产，LAYERTEC的飞秒镜片性能品质不仅十分出众，在功能方面也多种多样。
深圳维尔克斯光电是LAYERTECZG供应商，应其公司的所有型号系列。光学镜片应用波长范围从VUV（157nm）到NIR（4µm）。
LAYERTEC主要产品包括:各种波长的纳秒、皮秒、飞秒、连续激光反射镜，以及研究应用的激光滤光片，多功能宽带镜，负色散镜，GT干涉镜等
常应用于科研以及工业上基本所有的主流光学领域，镜片的材质也根据功能多种选择，有YAG,Sapphire,CaF2,IR-fused silica,Fused Silica,BK7，尺寸大部份为0.5英寸-2英寸。
NanosecondLaserOptics、Picosecond Laser Optics、Femtosecond Laser Optics
cw ａnd ns Laser Optics、Low Loss Laser Optics、Multipurpose Broadband Mirrors
Metallic Mirrors、 Filters for Laser Applications、Uncoated Optics
主要优点是：高透反率、低损耗和高损伤阈值。
飞秒激光光学元件按照其工作特行来划分，主要包含以下几类：
·标准飞秒激光光学元件·宽带飞秒激光光学元件·倍频程带宽飞秒光学元件
·银镜·高功率飞秒激光光学元件·钛蓝宝石倍频飞秒激光光学元件
·钛蓝宝石三倍频飞秒激光光学元件·钛蓝宝石高次谐波飞秒激光光学元件
·gires-tournois干涉仪镜·1100-1600nm飞秒激光激光光学元件
Layetec提供的纳秒激光反射镜规格如下：
| HR(0°,157nm)>=92% |
| HR(0°,193nm)>96% |
| HR(9°-12°,193nm)>96% |
| HRr(0°,260nm)>99.5% |
| HRr(0°,266nm)>99.5% |
| HR(0°,355nm)>99.9% |
| HR(0°,355nm)>99.85% |
| HRs,p(8.5°, 355nm)>99.75% + Rs,p(8.5°, 532nm)<0.5% + Rs,p(8.5°, 1064nm)<5% (high power) |
| HRs,p(0-20°, 355nm)>99% + HRs,p(0-20°, 532nm)>99% + Rs,p(0-20°, 1064nm)<1% |
| HR (0°, 515-532nm) >99,9% + R (0° , 1030-1064nm) <1% |
| HR(0-10°, 532nm)>99.8% + R(0-10°, 1064nm)<1% (High Power) |
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| HRr(45°,193nm)>95% |
| HRs(45°,213nm)>97% + Rp(45°,266nm)<2% + Rs(45°,532nm)<10% + Rp(45°,1064nm)<2% |
| HRr(45°, 248nm)>98% (fluoridic) |
| HRr(45°,248nm)>99% |
| HRr(45°,248nm)>99% + Rr(45°,355+848nm)<10% |
| HRs(45°,266nm)>99.5% + Rp(45°,532+1064nm)<2% + Rs(45°,532+1064nm)<10% |
| HRr(45°, 308nm)>99.5% |
| HRr(45°, 308nm)>99.8% |
| HRs(45°,343nm)>99.9% + Rp(45°,515nm)<0.2% + Rs(45°,1030nm)<0.2% |
| HRr(45°,351nm)>99.5% |
| HRr(45°, 355nm)>99.5% |
| HRr(45°, 355nm + 532nm)>99.5% |
| TFP(45°,355nm) Rs>99.5% Rp<2% |
| HRp(45°, 355nm)>99.8% + Rs(45°, 532nm)<1% + Rp(45°, 1064nm)<1% |
| HRs,p(45°, 532nm)>99.8% + Rs,p(45°, 1064nm)<2% (high power) |
| HRs,p(45°,1030nm)>99.96% (Zero Phase Shift) |
| HRr(45°,1030nm)>99.98% (High Power) |
| HRs(45°, 1030-1064nm)>99.9% (High Power) |
| HRr(45°, 1064nm)>99.9% |
| HRr(45°, 1064nm + 532nm)>99.8% + HRr(45°,355nm)>99.4% |
| HRr(45°,1064nm)>99.9% + Rr(45°,532nm)<10% |
| HRr(45°,1064nm)>99.9%+HTr(45°, 532+808nm)>90% |
| HRs(22.5°,343nm)>99.8% + Rp(22.5°,515nm)<1% + Rs(22.5°,1030nm)<1% |
| TFP(56°, 355nm) Rs>99.5% Rp<2% |
| TFP(56°(±3°)*, 532nm) Rs>99.8% Rp<2%, (±3°)* angle adjustment |
| PR(0°, 650-720nm)=80±5% + R(0°, 740-950nm)<10% (analogous F0305017) |
| PRr(45°,193nm)=30+/-3% |
| PRr(45°,248nm)=50±3% |
| PRs,p(45°,532nm)=50±5%, |Rs-Rp|<5% |
| PRp(45°, 1030-1064nm)=30.0±2% 由于字数限制，更多型号咨询可随时联系维尔克斯光电工作人员。
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| HR(0°,343nm)>99.7% + R(0°,515+1030nm)<1% (ps-pulses) | |
| HR(0°, 515nm)>99.9% (high power) | |
| HR(0°,532nm)>99.9% (High Power) | |
| HR(0°,750-850nm)>99.9% (high power for ps-pulses) | |
| HR(0°,970-1090nm)>99.9% (High Power for ps-Pulses) | |
| HRr(0-20°,970-1090nm)>99.95% (high power) | |
| HR(0°, 980-1090nm)>99.98% (High Power für ps-Pulse) | |
| HR(0°,990-1070nm)>99.98% (High Power für ps-Pulse) | |
| HR(0-10°, 1030±30nm)>99.98% (High Power ps-Pulse) | |
| HR(0°,1000-1100nm)>99.98% (High Power für ps-Pulse) | |
| HR(0°,1030nm)>99.98% (High Power) | |
| HR(0°,1030±30nm)>99.98% (High Power for ps-Pulses) | |
| HRr(0-20°,970-1090nm)>99.95% (high power for ps-pulses) | |
| HR(0°,1030-1064nm)>99.9% (High Power) | |
| HR(0°,1064nm)>99.98% (High Power für ps-Pulse) | |
| HRr(22.5°,1010-1070nm)>99.9% (High Power) | |
| Ag + Multilayer, HRr(0-45°, 1020-1040nm)>99.9% | |
| HRr(45°,213nm)>95% (HRs(45°,208-218nm)>97%, HRp(45°,213nm)>93%) (fluoridisch) | |
| HRs(45°,343nm)>99.9% + HRp(45°,343nm)>99.7% | |
| HRp(45°, 355nm)>99.0% + Rs(45°, 532nm)<3% + Rp(45°, 1064nm)<2% | |
| HRp(45°, 355nm)>99.5% + Rs(45°, 532nm)<5% + Rp(45°, 1064nm)<5% | |
| HRr(45°, 515nm)>99.9% (High Power for ps-pulses), T>0.05% | |
| HRs,p(45°,515nm)>99.9% (High Power für ps) | |
| HRs,p(45°,515nm)>99.9% + Rs,p(45°,1030nm)<2% | |
| HRs(45°,515nm)>99.95% + Rp(45°,1030nm)<1% (high power) | |
| HRr(45°,532nm)>99.9% (High Power for ps) | |
| HRr(45°,1030±40nm)>99.9% (High Power for ps-Pulses) | |
| HRr(45°, 1030±40nm)>99.9% (High Power für ps-Pulse), T>0.05% with HRr~99.95% => |Rs-Rp|~0.1% | |
| HRr(45°,990-1070nm)>99.98% (High Power für ps-Pulse) | |
| HRr(45°,1030±40nm)>99.9% + PRr(633-655nm)>80% (High Power für ps-Pulse) | |
| HRr(45°, 1030nm)>99.9% (High Power für ps-Pulse), T>0.05% | |
| HRr(45°, 1030nm)>99.98% (High Power for ps-pulses) | |
| HRr(45°, 1030nm + 515nm)>99.9% (high power) | |
| TFP(45°, 1030nm) Rs>99.9% Rp<2% | |
| TFP(55°, 1030nm), Rs>99.9%, Rp<1% | |
| PR(0°,1030nm)=75±2% | |
| PR(0°,1030nm)=77±2% | |
| PR(0°,1030nm)=79±2% | |
| PR(0°,1030nm)=81±2% | |
| PR(0°,1030nm)=83±2% | |
| PR(0°,1030nm)=85±2% | |
| PR(0°,1030nm)=87±2% | |
| 由于字数限制，更多型号咨询可随时联系维尔克斯光电工作人员。
三、飞秒激光反射镜 Femtosecond Laser Optics
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| HR(0°, 580-1020±10nm)>99.8%, GVD-oscillation(700-1000nm)~-100...0fs2 | |
| HR(0°, 580-1030±8nm)>99.9%, GVD(650-1000nm)~ -50fs2±20fs2 , (GVD-oszillation compensated) | |
| HR(0°, 580-1060±8nm)>99.8%, GDD - oscillation~-120...+40fs2 | |
| HR(0°, 600-700nm±6nm)>99.9%, GVD<20fs2 | |
| both mirrors: HR(0°, 600-900nm)>99.8%, GVD (600-900nm)~ -45fs2±20fs2, (GVD-Oscillation compensated, see data sheet) | |
| HR(0°, 600-930nm)>99.9%, GVD(700-950nm)~ -65±20fs2 (GVD-Oszillation compensated) | |
| HR(0°, 600-980nm)>99.9%, GVD(700-880nm)~-100fs2...+40fs2 | |
| HR(0°, 610-1030nm±10nm)>99.8% | |
| HR(0°, 620-720nm±5nm)>99.9% | |
| HR(0°, 620-900±8nm)>99.9%, GVD(700-900nm)~ -65±20fs2(GVD oscillation compensated) | |
| HR(0-12°, 620-1000±7nm)>99.8%, GVD(680-900nm)~-60±20fs2 | |
| HR(0°, 620-1000nm)>99.85%, GDD(0°, 700-1000nm)~ -50±20fs2, GDD - osz. compensated | |
| HR(0°, 620-1050nm)>=99.9% + R(0°, 490-540nm)<5%, GDD(680-1020nm)~ -50+/-20fs2, (GDD-oszillation compensated) | |
| HR(0°,620-1080nm)>99.9% + R(0°,488-532nm)<5% | |
| HR(0°, 620-1120±10nm)>99.9%, GD optimized | |
| HR(0°, 630-980nm)>99.7% + R(0°, 515-545nm)<10%, GDD(700-1020nm)~ -70+/-30fs2, (GDD-oszillation compensated) | |
| HR(0°, 630-1100±8nm)>99.8% + R(0°, 480-540nm)<10% | |
| HR(0°, 630-1140+/-10nm)>99.85%, GVD~-200fs2....100fs2 | |
| HR(0°, 630-1200nm)>99.8%, |GDD-R(0°, 650-1150nm)|<400fs2 | |
| HR(0°,640-1000nm)>99.8% + R(0°,(510-545)±5nm)<15%, GDD(720-1000nm)~ -70±30fs2, (GDD-oscillation compensated) | |
| HR(0°, 630-1000nm)>99.8% + R(0°, 510-550nm)<10%, GVD(720-1020nm)~ -70±30fs2 | |
| HR(0°, 640-1080+/-8nm)>99.9% + R(0°, 490-540+/-5nm)<5%, GVD~ -200...+100fs2 (GVD optimized for OPO-application) | |
| HR(0°, 650-860±7nm)>99.9%, GVD(770-795nm)~-550±75fs2 | |
| HR(0°, 650-900±5nm)>99.9%, GVD(700-900nm)~ -100±30fs2 , (GVD-oszillation compensated) | |
| HR(0°, 650-900±8nm)>99.9%, GVD~-150fs2....0fs2, with smoothed GD | |
| HR(0°, 650-1100nm)>99.8%, GD optimized | |
| HR(0°, 650-1070±8nm)>99.9%, GVD(740-980nm)=-70±30fs2 | |
| HR(0°,650-1100nm)>99.8% + R(0°,488-532nm)<5% | |
| HR(0°,660-980nm±10nm)>99.7% + R(0°,500-550nm)<5%, GVD~-50±20fs2(730-1000±10nm) | |
| HR(0°, 660-1050nm)>99.9%, High Power optimized (780-850nm) | |
| booth mirrors HR(0°, 660-1060nm)>99.8%, GDD(730-970nm)= -70±20fs2, (GDD-Oszillation compensated) | |
| HR(0°, 660-1100±9nm)>99.8%, GVD(740-1010nm)=-70±20fs2 | |
| HR(0°,660-1130nm±10nm)>99.9%, GVD(780-1010nm)~ -120fs2...+40fs2 | |
| HR(0°, 660-1130+/-8nm)>99.9% + R(0°, 510-550+/-5nm)<5%, GVD~ -200...0fs2 (GVD optimized for OPO-application) | |
| HR(0°,660-1150nm)>99.9% + R(0°,480-560nm)<5% | |
| HR(0°,670-1000nm)>99.8%, GVD(700-970nm)=-60±20fs2 | |
| HR(0-5°, 670-1020nm)>99.8%, GDD Osz. compens. (0-5°, 730-850nm) ~-500...+750±100fs2, TOD opt. | |
| HR(0-5°, 670-1040nm)>99.8%, GDD Osz. compens. (0-5°, 770-990nm) ~-120±30fs2 | |
| HR(0°, 680-890±7nm)>99.8%, GVD (0°, 720-880nm)~+100±30fs2 | |
| HR(0°, 680-890±7nm)>99.8%, GVD (0°, 720-880nm)~+80±30fs2 | |
| HR(0°,680-1100nm)>99.8%, not GVD optimized | |
| HR(0°,680-1100nm)>99.8% + HT(0°,488-532nm)>90% | |
| HR(0°,690-820nm)>99.9% + R(0°,488-532nm)<5%, GVD<20fs2 | |
| HR(0°,690-880nm±10nm )>99.9% + R(0°,500-550nm)<2%, GVD<20fs2 (710-870±10nm) | |
| HR(0°, 690-890±5nm)>99.9% + R(0°, 532nm)<2%, GDD(0°, 700-880±10nm)~0fs2 | |
| HR(0°,690-960nm±10nm)>99.9% + R(0°,500-540nm)<5%, GDD~0fs2(690-880±10nm) | |
| HR(0°,700-840nm)>99.95%, GVD<20fs2 | |
| HR(0°, 700-850nm)>99.8% + HT(0°, 514-532nm)>95%, GVD~0fs2 | |
| HR(0°,700-870±7nm)>99.9%, |GDD|<40fs2 | |
| HR(0°, 700-870±8nm)>99.9%, GDD=-40±15fs2(725-880nm) | |
| HR(0°, 700-880±8nm)>99.9% + R(0°, 450-550nm)<2%, GVD<20fs2 (710-870±8nm) | |
| HRr(0-45°,700-890±10nm)>99.9% (not GVD-optimized) | |
| HR(0°,700-900nm)>99.8%, GDD<40fs2 | |
| HR(0°,700-900nm)>99.9%, GVD(700-900)~ -50±20fs2 (GVD-oscillation compensated) | |
| HR(0°, 700-900nm)>99.9%, GVD(780-805nm)~-550±50fs2 | |
| HR(0°,700-900nm)>99.9%, GVD<40fs2 | |
| HR(0°,700-900nm)>99.8% + R(0°,532nm)<2%, GDD~0fs2 | |
| HR(0°, 700-950±5nm)>99.9% + R(0°, 505-535nm)<10%, GVD~ -50±20fs2(680-940±5nm) | |
| HR(0°, 700-970nm)>99.85%, GDD(700-950nm)~ -60....-30fs2 (GDD - oscillation compensated ａnd TOD optimized) | |
| HR(0°,700-980nm)>99.9% + R(0°,510-532nm)<10%, IGDD(R,0°,710-870nm)I<30fs2 | |
| HR(0°,700-1000nm)>99.9%, GDD-R(0°,700-1000nm)=-50±50fs2 | |
| HR(0°,700-1030nm)>99.8%, GVD(730-1000nm)=-60±20fs2 | |
| HR(0°, 705-920±8nm)>99.9%, GVD~-40±15fs2 | |
| HR(0°, 710-850±8nm)>99.9% + R(0°,350-400±5nm)<3% | |
| HR(0°,710-860nm)>99.9% + R(0°,480-570nm)<2%, GVD<20fs2 | |
| HR(0°, 710-880±5nm)>99.9%, GDD<20fs2 | |
由于字数限制，更多型号咨询可随时联系维尔克斯光电工作人员。
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