产品展示
代理：Layertec 飞秒激光镜片 纳秒、皮秒激光镜片 飞秒镜片推荐
点击次数：817发布时间：2017/6/12 15:34:34
更新日期：2018/8/25 11:36:41
所 在 地：中国大陆
产品型号：
优质供应
详细内容
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LAYERTEC中国供应商，专供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。
一、纳秒激光反射镜 Nanosecond Laser Optics
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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二、皮秒激光反射镜 Picosecond Laser Optics
| 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 | |
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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。
