Semrock公司是光學濾光片的，采用離子束濺射精確鍍膜工藝，產品具有高透過率，深度雜散光抑制，曲線陡直，損傷閾值高的特點。Semrock拉曼濾光片已成為，被廣泛的應用在共聚焦顯微拉曼、臺式拉曼和手持拉曼等儀器中。
Semrock公司是光學濾光片的，采用離子束濺射精確鍍膜工藝，產品具有高透過率，深度雜散光抑制，曲線陡直，損傷閾值高的特點。Semrock拉曼濾光片已成為，被廣泛的應用在共聚焦顯微拉曼、臺式拉曼和手持拉曼等儀器中。
| Semrock拉曼濾光片 | |
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| · Semrock RazorEdge截止拉曼濾光片 用于拉曼實驗的瑞利散射截止，可以實現低波數斯托克斯或反斯托克斯信號探測。 · Semrock RazorEdge二向色鏡 克服了傳統鍍膜的偏振態依賴性，從而具備和截止濾光片一樣的過渡帶陡度。它簡化了拉曼實驗的光路，搭配截止拉曼濾光片被廣泛的應用于拉曼探頭中。 · Semrock StopLine陷波濾光片 對于正反斯托克斯進行同時探測的拉曼實驗，StopLine陷波濾光片可以輕松勝任，同時比全息陷波濾光片更經濟。 · Semrock EdgeBasic經濟型截止拉曼濾光片 對于非低波數探測的拉曼實驗，可采用EdgeBasic系列截止拉曼濾光片。 · Semrock MaxLine激光純化濾光片 針對很多激光器(如半導體激光器)存在的光譜純度不足的情況，MaxLine系列窄帶激光純化濾光片，可有效的減小激光器縱模次峰對于拉曼信號的串擾。 |
| 型號 | 過渡帶寬 |
| LP03-325RE-25 LP03-325RU-25 | < 153 cm-1 < 305 cm-1 |
| LP02-355RE-25 LP02-355RU-25 | < 140 cm-1 < 279 cm-1 |
| LP02-407RU-25 | < 243 cm-1 |
| LP03-458RE-25 LP03-458RU-25 | < 109 cm-1 < 216 cm-1 |
| LP02-473RE-25 LP02-473RU-25 | < 105 cm-1 < 209 cm-1 |
| LP02-488RE-25 LP02-488RU-25 | < 102 cm-1 < 203 cm-1 |
| LP02-514RE-25 LP02-514RU-25 | < 97 cm-1 < 192 cm-1 |
| LP03-532RE-25 LP03-532RU-25 | < 90 cm-1 < 186 cm-1 |
| LP02-561RE-25 LP02-561RU-25 | < 89 cm-1 < 176 cm-1 |
| LP02-633RE-25 LP02-633RU-25 | < 79 cm-1 < 156 cm-1 |
| LP02-638RE-25 LP02-638RU-25 | < 78 cm-1 < 155 cm-1 |
| LP02-785RE-25 LP02-785RU-25 | < 63 cm-1 < 126 cm-1 |
| LP02-808RE-25 LP02-808RU-25 | < 62 cm-1 < 123 cm-1 |
| LP02-830RE-25 LP02-830RU-25 | < 60 cm-1 < 119 cm-1 |
| LP02-980RE-25 LP02-980RU-25 | < 51 cm-1 < 101 cm-1 |
| LP02-1064RE-25 LP02-1064RU-25 | < 47 cm-1 < 93 cm-1 |
| 型號 | 過渡帶寬 |
| SP01-532RU-25 | 186 cm-1 |
| SP01-561RU-25 | 176 cm-1 |
| SP01-633RU-25 | 160 cm-1 |
| SP01-785RU-25 | 129 cm-1 |
| 型號 | 過渡帶寬 |
| LPD01-355RU | < 279 cm-1 |
| LPD02-488RU | < 203 cm-1 |
| LPD02-514RU(停產) | < 192 cm-1 |
| LPD02-532RU | < 186 cm-1 |
| LPD02-633RU | < 156 cm-1 |
| LPD02-785RU | < 126 cm-1 |
| LPD02-830RU | < 119 cm-1 |
| LPD02-1064RU | < 93 cm-1 |
| 型號 | 激光波長nm | 帶寬 | OD |
| NF03-405E-25 | 405 | 9 nm | > 6 @ 405 nm |
| NF03-488E-25 | 488 | 14 nm | > 6 @ 488 nm |
| NF03-514E-25 | 514 | 16 nm | > 6 @ 514.5 nm |
| NF01-532U-25 NF03-532E-25 | 532 | 17 nm | > 6 @ 532 nm |
| NF03-561E-25 | 561 | 19 nm | > 6 @ 561.4 nm |
| NF03-594E-25 | 594 | 21.8 nm | > 6 @ 594.1 nm |
| NF03-633E-25 | 633 | 25 nm | > 6 @ 632.8 nm |
| NF03-658E-25 | 658 | 27 nm | > 6 @ 658 nm |
| NF03-785E-25 | 785 | 39 nm | > 6 @ 785 nm |
| NF03-808E-25 | 808 | 41 nm | > 6 @ 808 nm |
| 型號 | 過渡帶寬 | 透過率及范圍 |
| BLP01-325R-25 | 750.5 cm-1 | >93% 334.1 – 900.0 nm |
| BLP01-355R-25 | 687 cm-1 | >93% 364.9 – 900.0 nm |
| BLP01-364R-25 | 670 cm-1 | >93% 374.0 – 900.0 nm |
| BLP01-405R-25 | 595 cm-1 | >93% 421.5 – 900.0 nm |
| BLP01-442R-25 | 552 cm-1 | >93% 454.0 – 900.0 nm |
| BLP01-458R-25 | 552 cm-1 | >93% 470.7 – 900.0 nm |
| BLP01-473R-25 | 515 cm-1 | >93% 486.2 – 900.0 nm |
| BLP01-488R-25 | 497 cm-1 | >93% 504.7 – 900.0 nm |
| BLP01-514R-25 | 474 cm-1 | >93% 529.4 – 900.0 nm |
| BLP01-532R-25 | 458 cm-1 | >93% 546.9 – 900.0 nm |
| BLP02-561R-25 | 434.5 cm-1 | >93% 577.1 – 900.0 nm |
| BLP01-568R-25 | 429 cm-1 | >93% 584.1 – 900.0 nm |
| BLP01-594R-25 | 411 cm-1 | >93% 610.9 – 900.0 nm |
| BLP01-633R-25 | 385.4 cm-1 | >93% 650.5 – 1200.0 nm |
| BLP01-635R-25 | 380 cm-1 | >93% 660.0 – 1200.0 nm |
| BLP01-647R-25 | 377 cm-1 | >93% 665.2 -1200.0 nm |
| BLP01-664R-25 | 367 cm-1 | >93% 682.6 – 1200.0 nm |
| BLP01-785R-25 | 309 cm-1 | >93% 812.1 – 1200.0 nm |
| BLP01-808R-25 | 302 cm-1 | >93% 830.6 – 1600.0 nm |
| BLP01-830R-25 | 293.9 cm-1 | >93% 853.2 – 1600.0 nm |
| BLP01-980R-25 | 248.9 cm-1 | >93% 1007.4 – 1600.0 nm |
| BLP01-1064R-25 | 229 cm-1 | >93% 1093.8 – 1600.0 nm |
| BLP02-1319R-25 | 184.9 cm-1 | >93% 1355.9 – 2000.0 nm |
| BLP01-1550R-25 | 157 cm-1 | >93% 1593.4 – 2000.0 nm |
EdgeBasic經濟型低通拉曼濾光片
| 型號 | 過渡帶寬 | 透過率及范圍 |
| BSP01-532R-25 | 458 cm-1 | > 80% 350.0 – 400.0 nm > 93% 400.0 – 517.1 nm |
| BSP01-633R-25 | 385 cm-1 | > 80% 350.0 – 400.0 nm > 93% 400.0 – 615.1 nm |
| BSP01-785R-25 | 313 cm-1 | > 80% 350.0 – 400.0 nm > 93% 400.0 – 758.2 nm |
| 型號 | 帶寬 | 透過率 |
| LL01-248-12.5 LL01-248-25 | 1.7 nm (typ) 2.2 nm (max) | > 40% |
| LL01-266-12.5 LL01-266-25 | 1.9 nm (typ) 2.4 nm (max) | > 55% |
| LL01-325-12.5 LL01-325-25 | 1.2 nm (typ) 2.3 nm (max) | > 80% |
| LL01-355-12.5 LL01-355-25 | 1.3 nm (typ) 2.5 nm (max) | > 80% |
| LL01-364-12.5(停產) LL01-364-25(停產) | 1.4 nm (typ) 2.5 nm (max) | > 85% |
| LL01-372-12.5(停產) LL01-372-25(停產) | 1.4 nm (typ) 2.6 nm (max) | > 85% |
| LL01-407-12.5 LL01-407-25 | 1.5 nm (typ) 2.8 nm (max) | > 90% |
| LL01-442-12.5 LL01-442-25 | 1.7 nm (typ) 3.1 nm (max) | > 90% |
| LL01-458-12.5 LL01-458-25 | 1.7 nm (typ) 3.2 nm (max) | > 90% |
| LL01-488-12.5 LL01-488-25 | 1.9 nm (typ) 3.4 nm (max) | > 90% |
| LL01-491-12.5(停產) LL01-491-25(停產) | 1.9 nm (typ) 3.4 nm (max) | > 90% |
| LL01-514-12.5 LL01-514-25 | 2.0 nm (typ) 3.6 nm (max) | > 90% |
| LL01-532-12.5 LL01-532-25 | 2.0 nm (typ) 3.7 nm (max) | > 90% |
| LL01-543-12.5 LL01-543-25 | 2.1 nm (typ) 3.8 nm (max) | > 90% |
| LL02-561-12.5 LL02-561-25 | 2.1 nm (typ) 3.9 nm (max) | > 90% |
| LL01-568-12.5 LL01-568-25 | 2.2 nm (typ) 4 nm (max) | > 90% |
| LL01-633-12.5 LL01-633-25 | 2.4 nm (typ) 4.4 nm (max) | > 90% |
| LL01-647-12.5 LL01-647-25 | 2.5 nm (typ) 4.5 nm (max) | > 90% |
| LL01-671-12.5 LL01-671-25 | 2.6 nm (typ) 4.7 nm (max) | > 90% |
| LL01-780-12.5 LL01-780-25 | 3.0 nm (typ) 5.5 nm (max) | > 90% |
| LL01-785-12.5 LL01-785-25 | 3.0 nm (typ) 5.5 nm (max) | > 90% |
| LL01-808-12.5 LL01-808-25 | 3.1 nm (typ) 5.7 nm (max) | > 90% |
| LL01-810-12.5 LL01-810-25 | 3.1 nm (typ) 5.7 nm (max) | > 90% |
| LL01-830-12.5 LL01-830-25 | 3.2 nm (typ) 5.8 nm (max) | > 90% |
| LL01-852-12.5 LL01-852-25 | 3.2 nm (typ) 5.8 nm (max) | > 90% |
| LL01-976-12.5 LL01-976-25 | 3.7 nm (typ) 6.8 nm (max) | > 90% |
| LL01-980-12.5 LL01-980-25 | 3.7 nm (typ) 6.9 nm (max) | > 90% |
| LL01-1030-12.5 LL01-1030-25 | 3.9 nm (typ) 7.2 nm (max) | > 90% |
| LL01-1047-12.5 LL01-1047-25 | 4.0 nm (typ) 7.3 nm (max) | > 90% |
| LL01-1064-12.5 LL01-1064-25 | 4.0 nm (typ) 7.4 nm (max) | > 90% |
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