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Journal articles on the topic 'Collision spectroscopy'

To see the other types of publications on this topic, follow the link: Collision spectroscopy.

Author: Grafiati

Published: 4 June 2021

Last updated: 20 February 2023

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1

Mathur, D., C. Badrinathan, F. A. Rajgara, and U. T. Raheja. "State-Diagnosed Ion-Neutral Collisions leading to Charge Transfer." Symposium - International Astronomical Union 120 (1987): 27–28. http://dx.doi.org/10.1017/s0074180900153732.

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A significant reservoir of potential energy in hot astrophysical plasmas exists in multiply charged positive ions. Inelastic collisional processes involving such ions govern the ionization and energy balance in such plasmas. Although inelastic processes such as, charge transfer, have been widely investigated, there remains a paucity of knowledge about charge changing processes where both reactions and products are state-diagnosed. We have applied high-resolution translational energy gain/loss spectroscopy to investigate state-diagnosed collisions between Kr2+ and H2 leading to single electron capture into specific electronic states of Kr+ at collision energies in the range 1–6 keV.

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2

Stoneman, R. C., M. D. Adams, and T. F. Gallagher. "Resonant-collision spectroscopy of Rydberg atoms." Physical Review Letters 58, no. 13 (March 30, 1987): 1324–27. http://dx.doi.org/10.1103/physrevlett.58.1324.

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3

Andersen, Nils. "Collision Spectroscopy with Optically Prepared Targets." Physica Scripta T95, no. 1 (2001): 7. http://dx.doi.org/10.1238/physica.topical.095a00007.

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4

Zhang, Feifan, Jianping Wang, Zhigang Liu, Chao Zhai, and Jiaru Chu. "Collision possibility analysis and collision avoidance for multi-object fibre-fed spectrographs with theta–phi positioners." Monthly Notices of the Royal Astronomical Society 500, no. 1 (November 11, 2020): 101–8. http://dx.doi.org/10.1093/mnras/staa1944.

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ABSTRACT Multi-object spectroscopy has become a valuable technique in numerous modern astronomical facilities. Most spectrographs have thousands of fibre positioners packed at a focal plane with shared working space. Therefore, positioners might collide with each other, which can lead to them being damaged. In this study, we first analysed the types of collisions between hexagonal patterned theta–phi positioners and the possibility of these collisions. Based on this, we proposed a motion planning method by deploying a proposed ‘safety zone’ within the positioner patrol area. Simulated experiments validated that our method could completely solve collisions between positioners with equal arms, such as the Large-sky-Area Multi-Object fibre Spectroscopic Telescope (LAMOST) and the Dark Energy Spectroscopic Instrument (DESI), or between positioners with unequal arms, such as the Multi-Object Optical and Near-infrared Spectrograph (MOONS).

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5

Haller, Ivan, Urooj A. Mirza, and Brian T. Chait. "Collision induced decomposition of peptides. Choice of collision parameters." Journal of the American Society for Mass Spectrometry 7, no. 7 (July 1996): 677–81. http://dx.doi.org/10.1016/1044-0305(96)85613-3.

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6

Moneti, Gloriano, Simona Francese, Guido Mastrobuoni, Giuseppe Pieraccini, Roberta Seraglia, Giovanni Valitutti, and Pietro Traldi. "Do collisions inside the collision cell play a relevant role in CID-LIFT experiments?" Journal of Mass Spectrometry 42, no. 1 (January 2007): 117–26. http://dx.doi.org/10.1002/jms.1151.

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7

Druetta, M., T. Bouchama, S. Martin, and J. Désesquelles. "VUV Spectroscopy of Ar9+ and Kr9+ Low Energy Collision with H2." International Astronomical Union Colloquium 102 (1988): 365–68. http://dx.doi.org/10.1017/s0252921100108103.

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Photon spectroscopy of low energy collisions between multicharged ions and neutrals has opened new possibilities of wavelength and energy level determination since recent multicharged ion sources like the E.C.R. source, giving μA electric current of highly multicharged ions, are available.The experimental set-up has been already described (1.2) The ion beam is produced by an E.C.R. ion source. Light emitted as a result of the collision is observed at 25* to the beam axis with a 3m grazing incidence (82*) spectrometer equipped with a 300 or 600 lines/mm grating blazed at 55.2 or 27.6 nm respectively. The detection is realised by micro-channel plates (MCP). Typical beam currents are 0.45 and 0.40 μA for Kr9+and Ar9+respectively, through the 8 mm diameter entrance hole of the gas cell. The gas pressure was kept at 5 × 10−5mbar. The emission cross sections of all the new observed lines have been mesured. Taking into account the statistics; the error on the beam intensity due to double collisions; the errors on the pressure, on the relative efficiency curve of the spectrometer and on the absolute calibration; we may estimate the error bar to ± 30%.

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8

Snels, Marcel, Stefania Stefani, Angelo Boccaccini, David Biondi, and Giuseppe Piccioni. "A simulation chamber for absorption spectroscopy in planetary atmospheres." Atmospheric Measurement Techniques 14, no. 11 (November 17, 2021): 7187–97. http://dx.doi.org/10.5194/amt-14-7187-2021.

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Abstract. A novel simulation chamber, PASSxS (Planetary Atmosphere Simulation System for Spectroscopy), has been developed for absorption measurements performed with a Fourier transform spectrometer (FTS) and, possibly, a cavity ring-down (CRD) spectrometer with a sample temperature ranging from 100 up to 550 K, while the pressure of the gas can be varied from 10 mbar up to 60 bar. These temperature and pressure ranges cover a significant part of the planetary atmospheres in the solar system, and the absorption chamber can thus be used to simulate planetary atmospheres of solar planets and extrasolar planets with similar physical conditions. The optical absorption path for the FTS absorption measurements is 3.2 m due to the implementation of a multi-pass setup inside the chamber. The FTS measurements cover a wide spectral range, from the visible to the mid-infrared, with a sensitivity sufficient for medium-strength absorption bands. The FTS has been used previously to measure high-pressure atmospheres, including collision-induced absorption bands and continuum absorption at ambient temperatures. PASSxS allows the measurement of the temperature dependence of collision-induced bands and continuum absorption, which is important for both the modeling of planetary atmospheres and fundamental processes involving collisions between molecules and atoms.

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9

Bordas-Nagy, Jozsef, and Keith R. Jennings. "Collision-induced decomposition of ions." International Journal of Mass Spectrometry and Ion Processes 100 (October 1990): 105–31. http://dx.doi.org/10.1016/0168-1176(90)85071-9.

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10

Alexander, A. J., P. Thibault, and R. K. Boyd. "Collision-induced dissociation of Cs4I3+. An Example of Superelastic Collisions?" Rapid Communications in Mass Spectrometry 3, no. 8 (August 1989): 267–72. http://dx.doi.org/10.1002/rcm.1290030806.

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11

KAWAZUMI, Hirofumi, and Teiichiro OGAWA. "Elementary collision processes studied by laser spectroscopy." Review of Laser Engineering 18, no. 4 (1990): 241–49. http://dx.doi.org/10.2184/lsj.18.4_241.

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12

Dowek, D., J. C. Houver, C. Richter, and N. Andersen. "Collision spectroscopy with aligned and oriented atoms." Zeitschrift f�r Physik D Atoms, Molecules and Clusters 18, no. 3 (September 1991): 231–34. http://dx.doi.org/10.1007/bf01437076.

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13

Royer, T., D. Dowek, J. C. Houver, J. Pommier, and N. Andersen. "Collision spectroscopy with aligned and oriented atoms." Zeitschrift f�r Physik D Atoms, Molecules and Clusters 10, no. 1 (March 1988): 45–57. http://dx.doi.org/10.1007/bf01425580.

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14

Gong, Qi-huang, and Y. H. Zou. "Collision-enhanced Hanle resonances in absorption spectroscopy." Optics Communications 65, no. 1 (January 1988): 52–56. http://dx.doi.org/10.1016/0030-4018(88)90440-3.

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15

Madesis, I., A. Lagoyannis, M. Axiotis, T. J. Mertzimekis, M. Andrianis, E. P. Benis, S. Harissopulos, and T. J. M. Zouros. "APAPES - Atomic Physics with Accelerators: Projectile Electron Spectroscopy." HNPS Proceedings 21 (March 8, 2019): 153. http://dx.doi.org/10.12681/hnps.2022.

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The only existing heavy-ion accelerator in Greece, the 5.5 MV TANDEM at the National Research Center “Demokritos” in Athens has been used to date primarily for investigations centering around nuclear physics. Here, we propose to establish the new (for Greece) discipline of Atomic Physics with Accelerators, a strong field in the EU with important contributions to fusion, hot plasmas, astrophysics, accelerator technology and basic atomic physics of ion-atom collision dynamics, structure and technology. This will be accomplished by combining the existing interdisciplinary atomic collisions expertise from three Greek universities, the strong support of distinguished foreign researchers and the high technical ion-beam know-how of the TANDEM group into a cohesive initiative.Using the technique of Zero-degree Auger Projectile Spectroscopy (ZAPS), we shall complete a much needed systematic isoelectronic investigation of K-Auger spectra emitted from collisions of pre-excited ions with gas targets using novel techniques. Our results are expected to lead to a deeper understanding of the neglected importance of cascade feeding of metastable states [1] in collisions of ions with gas targets and further elucidate their role in the non-statistical production of excited three-electron states by electron capture, recently a field of conflicting interpretations awaiting further resolution.

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16

Devdariani A. Z. "Asymptotically spin forbidden quasimolecular radiative transitions (review)." Optics and Spectroscopy 130, no. 14 (2022): 2062. http://dx.doi.org/10.21883/eos.2022.14.53990.2609-21.

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Theoretical works on radiative transitions produced in thermal collisions of atoms of groups 2A, 12 of the periodic table with atoms of inert gases in the normal state as well as in nonsymmetrical collisions of inert gas atoms are discussed in the review. Such collisions are accompanied by either the decay or the population of the lower metastable state 3P2. The discussion has been carried out within the framework of analytical approaches based on the Fermi pseudopotential method and semiempirical method. The results on rate constants, absorption coefficients, radiative lifetimes, spectral profiles have been presented Keywords: optical collision spectroscopy, quasimolecular state interaction, Fermi pseudopotential, semi empirical procedure of term reconstruction.

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17

Andersson, G., and H. Morgner. "Impact collision ion scattering spectroscopy (ICISS) and neutral impact collision ion scattering spectroscopy (NICISS) at surfaces of organic liquids." Surface Science 405, no. 1 (May 1998): 138–51. http://dx.doi.org/10.1016/s0039-6028(98)00062-4.

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18

Alexander, A. J., P. Thibault, R. K. Boyd, J. M. Curtis, and K. L. Rinehart. "Collision induced dissociation of peptide ions." International Journal of Mass Spectrometry and Ion Processes 98, no. 2 (August 1990): 107–34. http://dx.doi.org/10.1016/0168-1176(90)85012-q.

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19

S., Shilpa, and Pramod Gopinath. "Study of stagnation layer of laterally colliding laser produced aluminium plasmas." IOP Conference Series: Materials Science and Engineering 1221, no. 1 (March 1, 2022): 012018. http://dx.doi.org/10.1088/1757-899x/1221/1/012018.

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Abstract When two dense laser produced plasmas collide, a layer of plasma stagnates at the collision front exhibiting special properties, is called stagnation layer. The characteristics of stagnation layer formed due to the collision of two laser produced aluminium plasmas were studied using spectroscopic and the fast imaging techniques. Time gated Intensified Charge Coupled Device (ICCD) imaging was used to study the temporal evolution of stagnation region and time resolved spectroscopy was used to obtain information about the distribution of neutral as well as the ionic species in collision process of laterally colliding aluminum plasmas. Electron density and temperature of the stagnation layer were also calculated from the emission spectra. The overall experiment results clearly depict the peculiar properties of stagnation layer which is more advantageous than the conventional laser produced plasma.

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20

Fannin, H. B., D. C. Miller, and C. J. Seliskar. "A Simple Kinetic Model for a Helium ICP." Applied Spectroscopy 41, no. 2 (February 1987): 173–76. http://dx.doi.org/10.1366/000370287774986778.

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A simple kinetic model is proposed to describe the population of the n3P and n1P states of helium for principle quantum numbers, n, from 3 to 10 in a 27-MHz ICP. The model incorporates two decay channels, namely those of radiative decay and collisional relaxation, to simulate the population. The functional form of the collision probability is approximated with the use of the Rydberg cross sections for the principal quantum number of the state. Experimental results are presented and are consistent with this model.

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21

Wang, M., A. Arnesen, R. Hallin, F. Heijkenskjöld, A. Langereis, M. O. Larsson, C. Nordling, and A. Wännström. "Collision-based spectroscopy of Xe viii Rydberg states." Journal of the Optical Society of America B 13, no. 8 (August 1, 1996): 1650. http://dx.doi.org/10.1364/josab.13.001650.

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22

Wang, M., M. O. Larsson, A. Arnesen, R. Hallin, F. Heijkenskjöld, C. Nordling, and A. Wännström. "Collision-based spectroscopy of Xe vi Rydberg states." Journal of the Optical Society of America B 13, no. 12 (December 1, 1996): 2715. http://dx.doi.org/10.1364/josab.13.002715.

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23

Mayo, M., D. Hitz, S. Dousson, J. P. Desclaux, and S. Bliman. "Charge-exchange-collision-based spectroscopy of Al VII." Journal of Physics B: Atomic and Molecular Physics 18, no. 16 (August 28, 1985): L539—L543. http://dx.doi.org/10.1088/0022-3700/18/16/001.

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24

Spitzl, Ralf, Horst Niehus, and George Comsa. "180° low‐energy impact collision ion scattering spectroscopy." Review of Scientific Instruments 61, no. 2 (February 1990): 760–64. http://dx.doi.org/10.1063/1.1141491.

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25

Wang, M., M. O. Larsson, A. Arnesen, R. Hallin, F. Heijkenskjöld, C. Nordling, and A. Wännstrüm. "Collision-based spectroscopy of Xe VI Rydberg states." Journal of the Optical Society of America B 14, no. 6 (June 1, 1997): 1515. http://dx.doi.org/10.1364/josab.14.001515.

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26

Wang, M., A. Arnesen, R. Hallin, F. Heijkenskjöld, A. Langereis, M. O. Larsson, C. Nordling, and A. Wännström. "Collision-based spectroscopy of Xe VIII Rydberg states." Journal of the Optical Society of America B 14, no. 6 (June 1, 1997): 1516. http://dx.doi.org/10.1364/josab.14.001516.

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27

Bortolini, O., M. Hamadan, and P. Traldi. "Investigation of singly charged dihalomethanes by collision spectroscopy." Rapid Communications in Mass Spectrometry 6, no. 1 (January 1992): 71–74. http://dx.doi.org/10.1002/rcm.1290060115.

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28

Teule, R., S. Stolte, and W. Ubachs. "Collision-Induced E(0g+)−D(0u+) State-to-State Energy Transfer in I2." Laser Chemistry 18, no. 3 (January 1, 1999): 111–28. http://dx.doi.org/10.1155/1999/86213.

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Electronic energy transfer in the E(0g+)−D(0u+) system of I2 is investigated in an experiment, where single rovibrational quantum states are prepared, single collision conditions prevail, and the final states have been determined from dispersed fluorescence. In I2∗(E)−X (X=Ar, N2, O2) the collisional decay is found to be governed by minimum energy transfer. With (X=I2) an anomalous behaviour is found for the initially prepared E, ν=8, J=56 level, which is tentatively ascribed to vibrational excitation of the collision partner.

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29

Voinov, Valery G., Max L. Deinzer, Joseph S. Beckman, and Douglas F. Barofsky. "Electron Capture, Collision-Induced, and Electron Capture-Collision Induced Dissociation in Q-TOF." Journal of The American Society for Mass Spectrometry 22, no. 4 (February 12, 2011): 607–11. http://dx.doi.org/10.1007/s13361-010-0072-x.

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30

Wang, Xin, Jun He, Jiandong Bai, and Junmin Wang. "Rydberg Level Shift due to the Electric Field Generated by Rydberg Atom Collision Induced Ionization in Cesium Atomic Ensemble." Applied Sciences 10, no. 16 (August 14, 2020): 5646. http://dx.doi.org/10.3390/app10165646.

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We experimentally studied the Rydberg level shift caused by the electric field, which is generated by Rydberg atom collision induced ionization in a cesium atomic ensemble. The density of charged particles caused by collisions between Rydberg atoms is changed by controlling the ground-state atomic density and optical excitation process. We measured the Rydberg level shift using Rydberg electromagnetically-induced-transparency (EIT) spectroscopy, and interpreted the physical origin using a semi-classical model. The experimental results are in good agreement with the numerical simulation. These energy shifts are important for the self-calibrated sensing of microwave field by the employing of Rydberg EIT. Moreover, in contrast to the resonant excitation case, narrow-linewidth spectroscopy with high signal-to-noise ratio would be useful for high-precision measurements.

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31

Tajima, Susumu, Low Foon Siang, Masao Fujishige, Satoshi Nakajima, and Osamu Sekiguchi. "Collision-induced dissociation spectra versus collision energy (collision-induced dissociation curve) using a quadrupole ion trap mass spectrometer. II.1 Loss of CO from ionizedo-,m- andp-anisoyl fluoride, CH3OC6H4COF+�." Journal of Mass Spectrometry 35, no. 9 (2000): 1144–46. http://dx.doi.org/10.1002/1096-9888(200009)35:9<1144::aid-jms43>3.0.co;2-q.

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32

Houver, J. C., D. Dowek, J. Pommier, and C. Richter. "Collision spectroscopy with aligned and oriented atoms. II. Charge exchange in He+-Na(3p) collisions." Journal of Physics B: Atomic, Molecular and Optical Physics 22, no. 20 (October 28, 1989): L585—L589. http://dx.doi.org/10.1088/0953-4075/22/20/002.

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33

Morris, Michael, Pierre Thibault, and Robert K. Boyd. "Characterization of a high-pressure quadrupole collision cell for low-energy collision-indneed dissociation." Journal of the American Society for Mass Spectrometry 5, no. 12 (December 1994): 1042–63. http://dx.doi.org/10.1016/1044-0305(94)85066-6.

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34

Bialecki, Jason B., Josef Ruzicka, Carl S. Weisbecker, Meena Haribal, and Athula B. Attygalle. "Collision-induced dissociation mass spectra of glucosinolate anions." Journal of Mass Spectrometry 45, no. 3 (March 2010): 272–83. http://dx.doi.org/10.1002/jms.1711.

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35

Flammang, Robert, Julien De Winter, Pascal Gerbaux, Vinh Son Nguyen, and Minh Tho Nguyen. "Internal Energy Effects on the Ion/Molecule Reactions of Ionized Methyl Isocyanide." European Journal of Mass Spectrometry 14, no. 5 (April 1, 2008): 299–309. http://dx.doi.org/10.1255/ejms.936.

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Electron ionization of methyl isocyanide in various chemical ionization conditions is reported and, depending on the energy conditions used, different ion/molecule reactions are observed. It is proposed, on the basis of combined quantum chemical (DFT) calculations and tandem mass spectrometric experiments, that a common intermediate could be a cumulenic ionized dimer dissociating in the ion source following two energy depending competitive channels, a loss of a hydrogen atom and a loss of a methyl group. Proposed structures for new cumulenic ions are supported by collision experiments in the high (collisional activation) or/and low (collision-induced dissociations) translational energy regime.

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36

Bayat, Parisa, Denis Lesage, and Richard B. Cole. "Low-energy collision-induced dissociation (low-energy CID), collision-induced dissociation (CID), and higher energy collision dissociation (HCD) mass spectrometry for structural elucidation of saccharides and clarification of their dissolution mechanism i." Journal of Mass Spectrometry 53, no. 8 (July 9, 2018): 705–16. http://dx.doi.org/10.1002/jms.4205.

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37

Zou, Y., M. Wang, R. Hutton, and F. Heijkensköld. "Collision based spectroscopy of Na- and Mg-like Argon." Physica Scripta T73 (January 1, 1997): 79–80. http://dx.doi.org/10.1088/0031-8949/1997/t73/021.

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38

Bliman, S., M. Cornille, B. A. Huber, H. Lebius, A. Langereis, J. Nordgren, and R. Bruch. "Collision spectroscopy ofAr8++H2at low velocities(v<1a.u.)." Physical Review A 60, no. 4 (October 1, 1999): 2799–807. http://dx.doi.org/10.1103/physreva.60.2799.

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39

Church, D. A., M. Druetta, R. Dunford, C. Froese-Fischer, M. Idrees, V. M. Umar, and C. J. Liu. "Collision spectroscopy of low-energy-beam U^5+ ions." Journal of the Optical Society of America B 9, no. 12 (December 1, 1992): 2159. http://dx.doi.org/10.1364/josab.9.002159.

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40

Lessen, Daniel, J. Spencer Baskin, Christopher M. Jones, Tian He, and Edwin Carrasquillo-Molina. "Collision-Assisted Spectroscopy of HCN above the Isomerization Barrier." Journal of Physical Chemistry A 107, no. 30 (July 2003): 5697–702. http://dx.doi.org/10.1021/jp021075n.

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41

Kawamoto, Kiyoshi, Kei Inari, Tatsuo Mori, and Kenjiro Oura. "A New Apparatus for Impact Collision Ion Scattering Spectroscopy." Japanese Journal of Applied Physics 34, Part 1, No. 9A (September 15, 1995): 4917–19. http://dx.doi.org/10.1143/jjap.34.4917.

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42

Beynon, John H., A. Gareth Brenton, and Robert K. Boyd. "Some applications of collision spectroscopy of gas-phase ions." Journal of the Chemical Society, Faraday Transactions 2 83, no. 1 (1987): 37. http://dx.doi.org/10.1039/f29878300037.

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43

Bott, Geoffrey, Sherri Ogden, and Julie A. Leary. "Collision-energy ramp. A modification to an RF-only quadrupole collision cell." Rapid Communications in Mass Spectrometry 4, no. 9 (September 1990): 341–44. http://dx.doi.org/10.1002/rcm.1290040909.

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44

Fabris, Daniele, Michele Kelly, Zhuchun Wu, Catherine Fenselau, and K. R. Jennings. "Collision energy effects on the collision-induced dissociation of multiply charged melittin." Rapid Communications in Mass Spectrometry 8, no. 9 (September 1994): 791–95. http://dx.doi.org/10.1002/rcm.1290080926.

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45

Brunger, MJ. "Recent Applications of (e, 2e) Techniques." Australian Journal of Physics 49, no. 2 (1996): 347. http://dx.doi.org/10.1071/ph960347.

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The flexibility of the (e, 2e) technique in obtaining information on both structure and collision dynamics is demonstrated. An example of the structure information that can be obtained is illustrated by electron momentum spectroscopy studies on krypton, while the role of post-collision effects and correlations is explored by measurements in the autoionising region of helium.

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46

Covey, T., and D. J. Douglas. "Collision cross sections for protein ions." Journal of the American Society for Mass Spectrometry 4, no. 8 (August 1993): 616–23. http://dx.doi.org/10.1016/1044-0305(93)85025-s.

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47

Eichelberger, Brian R., Theodore P. Snow, and Veronica M. Bierbaum. "Collision rate constants for polarizable ions." Journal of the American Society for Mass Spectrometry 14, no. 5 (May 2003): 501–5. http://dx.doi.org/10.1016/s1044-0305(03)00134-x.

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48

Lemoine, Jérôme, Bernard Fournet, Dominique Despeyroux, Keith R. Jennings, Raoul Rosenberg, and Edmond Hoffmann. "Collision-induced dissociation of alkali metal cationized and permethylated oligosaccharides: Influence of the collision energy and of the collision gas for the assignment of linkage position." Journal of the American Society for Mass Spectrometry 4, no. 3 (March 1993): 197–203. http://dx.doi.org/10.1016/1044-0305(93)85081-8.

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49

Raftery, Mark J., and John H. Bowie. "Collision-induced dissociations of enolate negative ions. Deprotonated cyclohexanones." International Journal of Mass Spectrometry and Ion Processes 79, no. 3 (November 1987): 267–85. http://dx.doi.org/10.1016/0168-1176(87)83005-7.

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50

Cooks, R. Graham. "Special feature: Historical. Collision-induced dissociation: Readings and commentary." Journal of Mass Spectrometry 30, no. 9 (September 1995): 1215–21. http://dx.doi.org/10.1002/jms.1190300902.

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