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Photoionization

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case of molecules, the photoionization cross-section can be estimated by examination of Franck-Condon factors between a ground-state molecule and the target ion. This can be initialized by computing the vibrations of a molecule and associated cation (post ionization) using quantum chemical software e.g. QChem. For photon energies below the ionization threshold, the photoionization cross-section is near zero. But with the development of pulsed lasers it has become possible to create extremely intense, coherent light where multi-photon ionization may occur via sequences of excitations and relaxations. At even higher intensities (around
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When either the laser intensity is further increased or a longer wavelength is applied as compared with the regime in which multi-photon ionization takes place, a quasi-stationary approach can be used and results in the distortion of the atomic potential in such a way that only a relatively low and
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Several photons of energy below the ionization threshold may actually combine their energies to ionize an atom. This probability decreases rapidly with the number of photons required, but the development of very intense, pulsed lasers still makes it possible. In the perturbative regime (below about
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which are separated by the photon energies, indicating that the emitted electron has more kinetic energy than in the normal (lowest possible number of photons) ionization case. The electrons released from the target will have approximately an integer number of photon-energies more kinetic energy.
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of the species – the probability of an ionization event conceptualized as a hypothetical cross-sectional area. This cross section depends on the energy of the photon (proportional to its wavenumber) and the species being considered i.e. it depends on the structure of the molecular species. In the
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Not every interaction between a photon and an atom, or molecule, will result in photoionization. The probability of photoionization is related to the
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Delone, N. B.; Krainov, V. P. (1998). "Tunneling and barrier-suppression ionization of atoms and ions in a laser radiation field".
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Deng, Z.; Eberly, J. H. (1985). "Multiphoton absorption above ionization threshold by atoms in strong laser fields".
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than the usual case of just-above threshold ionization. More precisely, the system will have multiple peaks in its
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Protopapas, M; Keitel, C H; Knight, P L (1 April 1997). "Atomic physics with super-high intensity lasers".
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Dichiara, A.; et al. (2005). "2005 Quantum Electronics and Laser Science Conference".
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Photoionization is the process that makes once-invisible filaments in deep space glow.
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Vacuum Ultraviolet Photoionization and Photodissociation of Molecules and Clusters
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or for larger distortions even overcome this barrier. These phenomena are called
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is the physical process in which an ion is formed from the interaction of a
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Proceedings of the Quantum Electronics and Laser Science Conference
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Photoabsorption, photoionization, and photoelectron spectroscopy
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10 W/cm at optical frequencies), the probability of absorbing
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Ion formation via a photon interacting with a molecule or atom
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and the continuum states remains. Then, the electron can
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(1979). 228:Compendium of Chemical Terminology 14: 1603: 1130: 995:Deep-level transient spectroscopy 747:Saturated absorption spectroscopy 1082: 1071: 1070: 1000:Dual-polarization interferometry 584: 47: 1015:Scanning tunneling spectroscopy 990:Circular dichroism spectroscopy 985:Acoustic resonance spectroscopy 276:10.1070/PU1998v041n05ABEH000393 61:of infrared or visible light), 944:Fourier-transform spectroscopy 632:Vibrational circular dichroism 407: 373:Reports on Progress in Physics 364: 327: 290: 245: 216: 191: 67:barrier suppression ionization 1: 742:Cavity ring-down spectroscopy 647:Thermal infrared spectroscopy 184: 54:photoionization cross section 876:Inelastic neutron scattering 7: 937:Data collection, processing 813:Photoelectron/photoemission 443:10.1103/PhysRevLett.42.1127 167: 162:over-the-barrier ionization 10: 1608: 1395:X-Ray Fluorescence Imaging 1283:Anomalous X-ray scattering 1022:Photoacoustic spectroscopy 964:Time-resolved spectroscopy 393:10.1088/0034-4885/60/4/001 303:Optical Society of America 128:Above-threshold ionization 122:excited intermediate state 1542: 1474: 1423: 1308: 1301: 1240: 1199: 1138: 1066: 1048:Astronomical spectroscopy 1040: 1027:Photothermal spectroscopy 977: 936: 929: 891: 863: 805: 755: 655: 592: 508:Joseph Berkowitz (1979). 311:10.1109/QELS.2005.1549346 148:narrow barrier between a 120:can be used to access an 1222:Synchrotron light source 203:ESA/Hubble Press Release 1241:Interaction with matter 1200:Sources and instruments 1032:Pump–probe spectroscopy 921:Ferromagnetic resonance 713:Laser-induced breakdown 533:V. S. Letokhov (1987). 421:Physical Review Letters 241:10.1351/goldbook.P04620 77:Multi-photon ionization 71:rescattering ionization 1373:Diffraction tomography 728:Glow-discharge optical 708:Raman optical activity 622:Rotational–vibrational 358:10.1364/JOSAB.2.000486 305:. pp. 1974–1976. 136:photoelectron spectrum 26: 1484:X-ray crystallography 1353:Soft x-ray microscopy 1321:Panoramic radiography 1161:Synchrotron radiation 949:Hyperspectral imaging 483:Cheuk-Yiu Ng (1991). 24: 1253:Photoelectric effect 1186:Characteristic X-ray 701:Coherent anti-Stokes 656:UV–Vis–NIR "Optical" 1273:Photodisintegration 1248:Rayleigh scattering 1227:Free-electron laser 1005:Hadron spectroscopy 795:Conversion electron 756:X-ray and Gamma ray 663:Ultraviolet–visible 434:1979PhRvL..42.1127A 385:1997RPPh...60..389P 350:1985JOSAB...2..486D 268:1998PhyU...41..469D 1514:X-ray reflectivity 1293:X-ray fluorescence 1258:Compton scattering 1191:High-energy X-rays 1053:Force spectroscopy 978:Measured phenomena 969:Video spectroscopy 673:Cold vapour atomic 539:. Academic Press. 65:phenomena such as 27: 1574: 1573: 1570: 1569: 1562:X-ray lithography 1494:Backscatter X-ray 1489:X-ray diffraction 1316:X-ray radiography 1288:X-ray diffraction 1181:Siegbahn notation 1098: 1097: 1062: 1061: 954:Spectrophotometry 881:Neutron spin echo 855:Beta spectroscopy 768:Energy-dispersive 546:978-0-12-444320-4 525:978-0-12-091650-4 500:978-981-02-0430-3 475:978-0-306-45038-9 428:(17): 1127–1130. 158:tunnel ionization 143:Tunnel ionization 1599: 1400:X-ray holography 1306: 1305: 1278:Radiation damage 1125: 1118: 1111: 1102: 1101: 1086: 1085: 1074: 1073: 934: 933: 845:phenomenological 594:Vibrational (IR) 579: 572: 565: 556: 555: 550: 529: 504: 491:World Scientific 479: 448: 447: 445: 411: 405: 404: 368: 362: 361: 331: 325: 324: 294: 288: 287: 249: 243: 220: 214: 213: 211: 209: 195: 164:, respectively. 63:non-perturbative 60: 1607: 1606: 1602: 1601: 1600: 1598: 1597: 1596: 1577: 1576: 1575: 1566: 1550:X-ray astronomy 1538: 1470: 1419: 1405:X-ray telescope 1297: 1268:Photoionization 1236: 1232:X-ray nanoprobe 1195: 1151:Absorption edge 1139:Characteristics 1134: 1129: 1099: 1094: 1058: 1036: 973: 925: 887: 859: 801: 751: 651: 612:Resonance Raman 588: 583: 553: 547: 526: 501: 476: 457: 455:Further reading 452: 451: 412: 408: 369: 365: 332: 328: 321: 301:. 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Retrieved 202: 193: 146: 126: 106:spectroscopy 100: 96:Stark effect 91: 87: 83: 80: 70: 66: 59:10 – 10 W/cm 51: 29: 28: 18: 1217:Synchrotron 627:Vibrational 150:bound state 116:in which a 1592:Ionization 1581:Categories 1476:Scattering 1341:Helical CT 1207:X-ray tube 833:Two-photon 735:absorption 617:Rotational 344:(3): 491. 185:References 179:Radiolysis 174:Ion source 112:and small 911:Terahertz 892:Radiowave 790:Mössbauer 401:250856994 114:molecules 1212:Betatron 1077:Category 806:Electron 773:Emission 723:emission 680:Vibronic 284:94362581 208:23 April 168:See also 42:molecule 36:with an 1555:History 1309:Imaging 1089:Commons 916:ESR/EPR 864:Nucleon 692:(REMPI) 430:Bibcode 381:Bibcode 346:Bibcode 264:Bibcode 1543:Others 1504:GISAXS 1176:L-edge 1171:K-edge 930:Others 718:Atomic 543:  522:  497:  472:  399:  317:  282:  34:photon 1534:EDXRD 1456:XANES 1451:EXAFS 1441:ARPES 1388:3DXRD 1146:X-ray 871:Alpha 840:Auger 818:X-ray 785:Gamma 763:X-ray 696:Raman 607:Raman 602:FT-IR 397:S2CID 280:S2CID 223:IUPAC 110:atoms 1519:RIXS 1509:WAXS 1499:SAXS 1410:DFXM 1378:XDCT 1363:STXM 1358:XPCI 1346:XACT 541:ISBN 520:ISBN 495:ISBN 470:ISBN 315:ISBN 210:2015 160:and 69:and 38:atom 1524:XRS 1466:XFH 1461:EDS 1446:AES 1436:XPS 1431:XAS 1415:DXA 1383:DCT 1331:CDI 899:NMR 438:doi 389:doi 354:doi 307:doi 272:doi 237:doi 235:". 108:of 90:as 40:or 1583:: 1529:XS 1336:CT 904:2D 823:UV 518:. 514:. 493:. 489:. 436:. 426:42 424:. 418:. 395:. 387:. 377:60 375:. 352:. 340:. 313:. 278:. 270:. 260:41 258:. 225:, 201:. 124:. 98:. 44:. 1124:e 1117:t 1110:v 578:e 571:t 564:v 549:. 528:. 503:. 478:. 446:. 440:: 432:: 403:. 391:: 383:: 360:. 356:: 348:: 342:2 323:. 309:: 286:. 274:: 266:: 239:: 212:. 92:I 88:I 84:N

Index


photon
atom
molecule
photoionization cross section
non-perturbative
Stark effect
Resonance-enhanced multiphoton ionization
spectroscopy
atoms
molecules
tunable laser
excited intermediate state
Above-threshold ionization
kinetic energy
photoelectron spectrum
bound state
tunnel through
tunnel ionization
over-the-barrier ionization
Ion source
Radiolysis
"Hubble finds ghosts of quasars past"
IUPAC
Compendium of Chemical Terminology
photoionization
doi
10.1351/goldbook.P04620
Physics-Uspekhi
Bibcode

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