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Harmonic generation

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1471: 20: 632:(5HG) or more is theoretically possible, but the interaction requires a very high number of photons to interact and has therefore a low probability to happen: the signal at higher harmonics will be very low, and requires very intense lasers to be generated. To generate high harmonics (like 1077:
Kojima, Tetsuo; Konno, Susumu; Fujikawa, Shuichi; Yasui, Koji; Yoshizawa, Kenji; Mori, Yusuke; Sasaki, Takatomo; Tanaka, Mitsuhiro; Okada, Yukikatsu (2000). "20-W ultraviolet-beam generation by fourth-harmonic generation of an all-solid-state laser".
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Because the process requires that many photons are present at the same time and at the same place, the generation process has a low probability to occur, and this probability decreases with the order
181: 551: 457: 306: 279: 420: 366: 601: 656: 630: 518: 400: 346: 252: 204: 131: 103: 83: 60: 1051: 520:. Reported around the year 2000, powerful lasers now enable efficient FHG. This process involves the 4th order nonlinear susceptibility 1431: 1061: 744: 723: 875: 848: 815: 704: 683: 694: 1170: 734: 1340: 1007:
Cheng, Ji-Xin; Xie, X. Sunney (2002). "Green's function formulation for third-harmonic generation microscopy".
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Unlike SHG, it is a volumetric process and has been shown in liquids. However, it is enhanced at interfaces.
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with the same frequency interact with a nonlinear material, are "combined", and generate a new photon with
1396: 865: 673: 1200: 765: 317: 210:, for instance), and the light source must be intense and well-controlled spatially (with a collimated 1495: 206:. To generate efficiently, the symmetry of the medium must allow the signal to be amplified (through 891:
Moreaux, Laurent; Sandre, Olivier; Charpak, Serge; Blanchard-Desce, Mireille; Mertz, Jerome (2001).
770: 659: 223: 142: 348:. Also a special case of sum-frequency generation in which both photons are at the same frequency 148: 523: 429: 284: 257: 1370: 1190: 1258: 405: 351: 795: 580: 1365: 1248: 1236: 1163: 1087: 1016: 965: 904: 635: 8: 1416: 1335: 1275: 1195: 609: 576: 497: 379: 325: 231: 1091: 1020: 969: 908: 933: 892: 821: 807: 189: 116: 88: 68: 45: 916: 1436: 1310: 1285: 1111: 1103: 1057: 1032: 989: 981: 938: 920: 871: 844: 811: 796: 740: 719: 700: 679: 483: 825: 1446: 1411: 1391: 1360: 1095: 1024: 973: 928: 912: 803: 760: 423: 39: 1474: 1355: 1345: 1156: 1451: 1441: 1401: 1350: 1268: 1221: 1205: 207: 486:
can convert THG, otherwise THG can be generated from membranes in microscopy.
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is preferred. This process involves the 3rd order nonlinear susceptibility
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Kajzar, F.; Messier, J. (1985). "Third-harmonic generation in liquids".
1305: 183:), the medium must have no center of symmetry (non-centrosymmetrical). 110: 1421: 1263: 1243: 1226: 106: 1129: 376:
A special case in which the number of photons in the interaction is
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A special case in which the number of photons in the interaction is
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A special case in which the number of photons in the interaction is
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A special case in which the number of photons in interaction is
62: 214:) and temporally (more signal if the laser has short pulses). 145:, harmonic generation is possible. Note that for even orders ( 1179: 211: 489: 1148: 794:
Boyd, R. (2007). "The Nonlinear Optical Susceptibility".
1076: 893:"Coherent Scattering in Multi-Harmonic Light Microscopy" 422:. If they have different frequency, the general term of 85:
times the energy of the initial photons (equivalently,
638: 612: 583: 526: 500: 432: 408: 382: 354: 328: 287: 260: 234: 192: 151: 119: 91: 71: 48: 658:and so on), the substantially different process of 311: 1050:Pavone, Francesco S.; Campagnola, Paul J. (2016). 650: 624: 595: 545: 512: 451: 414: 394: 371: 360: 340: 300: 273: 246: 198: 175: 125: 97: 77: 54: 217: 1487: 1049: 949: 884: 732: 254:, but with two different photons at frequencies 1053:Second Harmonic Generation Imaging, 2nd edition 1070: 1164: 955: 402:, if all the photons have the same frequency 1009:Journal of the Optical Society of America B 1000: 733:Zernike, Frits; Midwinter, John E. (2006). 1171: 1157: 838: 692: 932: 832: 556: 465: 1006: 18: 1432:Multiple-prism grating laser oscillator 787: 490:Fourth-harmonic generation (FHG or 4HG) 1488: 1152: 713: 863: 793: 671: 857: 13: 808:10.1016/B978-0-12-369470-6.00001-0 136: 14: 1507: 802:(third ed.). pp. 1–67. 141:In a medium having a substantial 1470: 1469: 718:(4th ed.). Addison-Wesley. 312:Second-harmonic generation (SHG) 839:Sutherland, Richard L. (2003). 693:Sutherland, Richard L. (2003). 372:Third-harmonic generation (THG) 1341:Amplified spontaneous emission 1122: 1043: 538: 532: 444: 438: 218:Sum-frequency generation (SFG) 1: 917:10.1016/S0006-3495(01)76129-2 781: 870:(third ed.). Elsevier. 841:Handbook of Nonlinear Optics 776:Optical frequency multiplier 696:Handbook of Nonlinear Optics 678:(third ed.). Elsevier. 176:{\displaystyle n=2,4,\dots } 36:multiple harmonic generation 7: 1397:Chirped pulse amplification 843:(2nd ed.). CRC Press. 754: 699:(2nd ed.). CRC Press. 546:{\displaystyle \chi ^{(4)}} 470:Nonlinear crystals such as 452:{\displaystyle \chi ^{(3)}} 301:{\displaystyle \omega _{2}} 274:{\displaystyle \omega _{1}} 10: 1512: 1201:List of laser applications 1178: 1056:. CRC Taylor&Francis. 766:Second-harmonic generation 665: 318:Second-harmonic generation 315: 221: 1465: 1379: 1326: 1214: 1186: 16:Nonlinear optical process 978:10.1103/PhysRevA.32.2352 771:High harmonic generation 736:Applied Nonlinear Optics 660:high harmonic generation 606:Harmonic generation for 577:Harmonic generation for 224:Sum-frequency generation 143:nonlinear susceptibility 23:N-th harmonic generation 1029:10.1364/JOSAB.19.001604 415:{\displaystyle \omega } 361:{\displaystyle \omega } 1191:List of laser articles 739:. Dover Publications. 714:Hecht, Eugene (2002). 652: 626: 597: 596:{\displaystyle n>4} 557:Materials used for FHG 547: 514: 466:Materials used for THG 453: 416: 396: 362: 342: 302: 275: 248: 200: 177: 127: 99: 79: 56: 24: 653: 627: 598: 548: 515: 454: 417: 397: 363: 343: 303: 276: 249: 201: 178: 128: 100: 80: 57: 22: 1366:Population inversion 1100:10.1364/OL.25.000058 651:{\displaystyle n=30} 636: 610: 581: 573:) are used for FHG. 524: 498: 430: 406: 380: 352: 326: 285: 258: 232: 190: 149: 117: 89: 69: 46: 1417:Laser beam profiler 1336:Active laser medium 1276:Free-electron laser 1196:List of laser types 1092:2000OptL...25...58K 1021:2002JOSAB..19.1604C 970:1985PhRvA..32.2352K 909:2001BpJ....80.1568M 897:Biophysical Journal 864:Boyd, R.W. (2007). 672:Boyd, R.W. (2007). 625:{\displaystyle n=5} 513:{\displaystyle n=4} 395:{\displaystyle n=3} 341:{\displaystyle n=2} 247:{\displaystyle n=2} 28:Harmonic generation 648: 622: 593: 543: 510: 449: 412: 392: 358: 338: 298: 271: 244: 196: 173: 123: 95: 75: 52: 25: 1483: 1482: 1437:Optical amplifier 1286:Solid-state laser 1063:978-1-4398-4914-9 958:Physical Review A 199:{\displaystyle n} 126:{\displaystyle n} 98:{\displaystyle n} 78:{\displaystyle n} 55:{\displaystyle n} 42:process in which 40:nonlinear optical 1503: 1496:Nonlinear optics 1473: 1472: 1447:Optical isolator 1412:Injection seeder 1392:Beam homogenizer 1371:Ultrashort pulse 1361:Lasing threshold 1173: 1166: 1159: 1150: 1149: 1144: 1143: 1141: 1140: 1126: 1120: 1119: 1074: 1068: 1067: 1047: 1041: 1040: 1004: 998: 997: 964:(4): 2352–2363. 953: 947: 946: 936: 903:(3): 1568–1574. 888: 882: 881: 867:Nonlinear optics 861: 855: 854: 836: 830: 829: 801: 798:Nonlinear optics 791: 761:Nonlinear optics 750: 729: 710: 689: 675:Nonlinear optics 657: 655: 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Retrieved 1133: 1124: 1086:(1): 58–60. 1083: 1079: 1072: 1052: 1045: 1012: 1008: 1002: 961: 957: 951: 900: 896: 886: 866: 859: 840: 834: 797: 789: 735: 715: 695: 674: 605: 560: 493: 469: 461: 375: 321: 227: 185: 140: 35: 31: 27: 26: 1457:Q-switching 1318:X-ray laser 1311:Ti-sapphire 1281:Laser diode 1259:Helium–neon 1015:(7): 1604. 113:divided by 1139:2019-12-01 1134:raicol.com 782:References 111:wavelength 105:times the 1422:M squared 1244:Gas laser 1227:Dye laser 1108:0146-9592 1037:0740-3224 986:0556-2791 925:0006-3495 529:χ 435:χ 410:ω 356:ω 290:ω 263:ω 171:… 107:frequency 1490:Category 1475:Category 1269:Nitrogen 1116:18059781 943:11222317 826:15660817 755:See also 109:and the 1254:Excimer 1088:Bibcode 1017:Bibcode 994:9896350 966:Bibcode 934:1301348 905:Bibcode 666:Sources 63:photons 38:) is a 1296:Nd:YAG 1291:Er:YAG 1232:Bubble 1180:Lasers 1114:  1106:  1060:  1035:  992:  984:  941:  931:  923:  874:  847:  824:  814:  743:  722:  716:Optics 703:  682:  565:(β-BaB 474:(β-BaB 1301:Raman 822:S2CID 561:Some 482:) or 212:laser 1306:Ruby 1112:PMID 1104:ISSN 1058:ISBN 1033:ISSN 990:PMID 982:ISSN 939:PMID 921:ISSN 872:ISBN 845:ISBN 812:ISBN 741:ISBN 720:ISBN 701:ISBN 680:ISBN 588:> 281:and 1264:Ion 1096:doi 1025:doi 974:doi 929:PMC 913:doi 804:doi 563:BBO 553:. 484:LBO 472:BBO 133:). 1492:: 1132:. 1110:. 1102:. 1094:. 1084:25 1082:. 1031:. 1023:. 1013:19 1011:. 988:. 980:. 972:. 962:32 960:. 937:. 927:. 919:. 911:. 901:80 899:. 895:. 820:. 810:. 646:30 459:. 368:. 308:. 32:HG 1172:e 1165:t 1158:v 1142:. 1118:. 1098:: 1090:: 1066:. 1039:. 1027:: 1019:: 996:. 976:: 968:: 945:. 915:: 907:: 880:. 853:. 828:. 806:: 749:. 728:. 709:. 688:. 643:= 640:n 620:5 617:= 614:n 591:4 585:n 571:4 569:O 567:2 539:) 536:4 533:( 508:4 505:= 502:n 480:4 478:O 476:2 445:) 442:3 439:( 390:3 387:= 384:n 336:2 333:= 330:n 294:2 267:1 242:2 239:= 236:n 194:n 168:, 165:4 162:, 159:2 156:= 153:n 121:n 93:n 73:n 50:n 30:(

Index


nonlinear optical
photons
frequency
wavelength
nonlinear susceptibility
phase matching
laser
Sum-frequency generation
Second-harmonic generation
four-wave mixing
BBO
LBO
BBO
high harmonic generation
Nonlinear optics
ISBN
9780123694706
Handbook of Nonlinear Optics
ISBN
9780824742430
ISBN
978-0805385663
Applied Nonlinear Optics
ISBN
978-0486453606
Nonlinear optics
Second-harmonic generation
High harmonic generation
Optical frequency multiplier

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