Gotowe bibliografie tematyczne / Laser excited states of sodium

Gotowa bibliografia na temat „Laser excited states of sodium”

Autor: Grafiati

Data publikacji: 4 czerwca 2021

Data aktualizacji: 3 lutego 2022

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Artykuły w czasopismach na temat "Laser excited states of sodium"

Vušković, L. "Experiments with low-energy electrons scattered by polarized, excited sodium". Canadian Journal of Physics 74, nr 11-12 (1.11.1996): 991–96. http://dx.doi.org/10.1139/p96-819.

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Several crossed-beam experiments were performed to acquire information concerning collisions of low-impact-energy electrons with ground-state or laser-excited sodium atoms prepared in 32P3/2, F = 3 (MF = +3 or −3) polarized states. Results of these experiments are the azimuthal asymmetry of the differential cross sections between two polarized states in the elastic electron collision (3P → 3P) at selected scattering angles, absolute differential cross sections for elastic, inelastic, and superelastic scattering obtained with no normalization procedure involved, and total ionization cross sections in the threshold energy range.

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Hall, B. V., R. T. Sang, M. Shurgalin, W. R. MacGillivray, M. C. Standage i P. M. Farrell. "Electron superelastic scattering from states of atomic sodium and rubidium". Canadian Journal of Physics 74, nr 11-12 (1.11.1996): 977–83. http://dx.doi.org/10.1139/p96-817.

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This paper reports on the extension of the electron superelastic scattering technique to three new situations. The first considers scattering from the 32P3/2 level of Na that has been excited by two laser modes tuned, respectively, to the transitions from the two hyperfine states of the 32S1/2 ground level. Both coherent and noncoherent modes are treated in a full quantum electrodynamic model of the laser excitation. Under certain conditions, the time-averaged probability of finding an atom in the 32P3/2 level exceeds 0.5. The second situation is electron superelastic scattering from the 32D5/2 level of Na that has been resonantly excited from the ground level via a resonant intermediate level. With the first observation of superelastically scattered electrons from this higher lying level recently recorded, this paper considers the extension of the quantum electrodynamics (QED) model to describe the optical excitation process. Application of superelastic scattering to the 52S1/2–52P3/2 transition of Rb is the third situation considered. The superelastic scattering formalism is extended to allow for a nonzero spin flip cross section for this transition. The resulting optical pumping terms are calculated using the QED model and the method of their determination for the superelastic scattering experiment described. The experimental design necessary to measure all of the collision parameters for this transition is discussed.

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Ferray, M., F. Gounand, P. D’Oliveira, P. R. Fournier, D. Cubaynes, J. M. Bizau, T. J. Morgan i F. J. Wuilleumier. "Three-step excitation of highly excited autoionizing states in atomic sodium by use of laser beams and synchrotron radiation". Physical Review Letters 59, nr 18 (2.11.1987): 2040–43. http://dx.doi.org/10.1103/physrevlett.59.2040.

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Weigold, Erich. "(e,2e) Studies of Atoms ? Some Recent Developments". Australian Journal of Physics 43, nr 5 (1990): 543. http://dx.doi.org/10.1071/ph900543.

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Some recent work on (e,2e) collisions in atoms is reported. The first (e,2e) results on an excited target and also on an oriented target are discussed. Sodium atoms are pumped to the m/ = +1 state of the excited 3p state by 0"+ light from a laser. The (e,2e) measurements are then performed on this excited state. The results are in excellent agreement with the momentum density profile given by the 3p(m/ = 1) Hartree-Fock wavefunction. High resolution electron momentum spectroscopy measurements are reported for argon. The first momentum profiles for excited Ar ion states belonging to the 2po and 20e manifolds are obtained. The latter are entirely due to initial state correlations. Comparison is made with several many-body calculations. The importance of core quadrupole (10) excitations is demonstrated. Although the 2se manifold is dominated by final state correlations, the momentum profile to the 4s 2S ion state in the 2Se manifold also shows the influenee of initial state correlation effects. The third series of measurements examines correlations in the autoionising region of helium, encompassing the (2s2)1 S, (2s2p)3p, (2p2)! 0 and (2s2p)! P resonances, at 100, 200 and 400 eV incident electron energies. Measurements, with an energy resolution of 150 meV, were taken at a number of scattered electron angles over an extended range of ejected electron angles, encompassing both the binary and recoil regions. The data show very strong correlations between the resonance amplitudes and the direct ionisation amplitudes.

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Gulam, Rabbani M., Saburo Neya i Junji Teraoka. "Resonance Raman spectra of highly reduced iron porphycenes". Journal of Porphyrins and Phthalocyanines 10, nr 11 (listopad 2006): 1271–84. http://dx.doi.org/10.1142/s1088424606000648.

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The redox behavior of iron porphycenes using the sodium mirror contact technique is reported. The resonance Raman spectra are obtained for each redox state, in order to explore the vibrational characteristics of these species in different redox states. The observed resonance Raman behavior of Fe II porphycene anion radical and its dianion is interpreted using the vibrational analysis of free-base porphycene anion radical and dianion. For the first time, a species generated in the fourth reduction step, is confirmed by UV-vis spectroscopy and is assigned to Fe I porphycene π dianion. The dependence of resonance enhancements of Raman bands for the Fe I porphycene π dianion on excitation laser reveals structural distortion along the NC a C a N or C b C a C a C b segments of the pyrrole-pyrrole direct connection in the excited electronic state.

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Awang, Asmahani, S. K. Ghoshal, M. R. Sahar i R. Arifin. "Effect of Au NPs on the Spectral Modification of Er-Doped Zinc Sodium Tellurite Glass". Materials Science Forum 846 (marzec 2016): 45–51. http://dx.doi.org/10.4028/www.scientific.net/msf.846.45.

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Optimizing of the spectroscopic features of rare earth (RE) doped inorganic glasses via tuneable growth of metallic nanoparticles (NPs) is demanding in plasmonic based nanophotonics. We report the gold (Au) NPs assisted sizeable enhancements in Er3+ luminescence in zinc-sodium tellurite glass. Glasses of the form 70TeO2-20ZnO-10Na2O-(x)Er2O3-(y)Au (x = 0.0 and 1.0 mol%; y = 0.0-0.6 mol% in excess) are synthesized via melt-quenching method and thoroughly characterized. Au concentration dependent variations in the physical and spectroscopic properties of glasses are determined. XRD data confirms the amorphous nature of all samples. UV-Vis-NIR spectra reveal seven absorption bands corresponding to the transitions from ground state (4I15/2) to 4I13/2, 4I11/2, 4I9/2, 4F9/2, 2H11/2, 4F7/2 and 4F5/2 excited states of Er3+. TEM micrograph manifests the existence of non-spherical Au NPs with average size of 8.6 nm. Prominent surface plasmon band of Au NPs is evidenced around 629 nm. Furthermore, Au NPs display a SPR mediated strong absorption in the visible region. Room temperature visible down-conversion emission (under 425 nm excitation) reveal three significant peaks centred at 532 (moderate green represent 2H11/2 → 4I15/2 transition), 550 (weak green represent 4S3/2 → 4I15/2 transition) and 588 nm (strong green represent 4S3/2 → 4I15/2 transition). Glass containing 0.4 mol% of Au exhibiting the highest luminescence intensity is ascribed to the NPs local field enhancement and energy transfer between RE ions and NPs. Variations in the physical properties of glass are explained in terms of the alteration in structures and ligand interactions with Au NPs present in the glass network. The intense field amplification discerned in the vicinity of Au NPs is attributed to the charge accumulation at the surface of the NPs. Surface plasmon resonance (SPR) of Au NPs and energy transfer (ET) from NPs to Er3+ ions are primarily attributed for the observed spectral modification. It is established that our glass composition displaying such significant enhancement may be beneficial for the development of up-converted solid state lasers and other plasmonic devices.

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Schulz, Claus Peter, Christiana Bobbert, Taku Shimosato, Kota Daigoku, Nobuaki Miura i Kenro Hashimoto. "Electronically excited states of sodium–water clusters". Journal of Chemical Physics 119, nr 22 (8.12.2003): 11620–29. http://dx.doi.org/10.1063/1.1624599.

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BORDAS, C., P. BREVET, M. BROYER, J. CHEVALEYRE, P. LABASTIE i J. P. PERROT. "AUTOIONIZATION LIFETIMES IN LASER EXCITED Na2RYDBERG STATES". Le Journal de Physique Colloques 48, nr C7 (grudzień 1987): C7–651—C7–653. http://dx.doi.org/10.1051/jphyscol:19877157.

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Tan, W. S., Z. Shi, C. H. Ying i L. Vušković. "Electron-impact ionization of laser-excited sodium atom". Physical Review A 54, nr 5 (1.11.1996): R3710—R3713. http://dx.doi.org/10.1103/physreva.54.r3710.

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Kushawaha, V. S. "Associative ionization of laser excited Rydberg sodium-atoms". Physica B+C 132, nr 2 (lipiec 1985): 295–98. http://dx.doi.org/10.1016/0378-4363(85)90074-9.

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Rozprawy doktorskie na temat "Laser excited states of sodium"

Sang, Robert Thomas, i n/a. "Superelastic Electron Scattering from Laser Excited States of Sodium". Griffith University. School of Science, 1995. http://www4.gu.edu.au:8080/adt-root/public/adt-QGU20050921.120911.

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This thesis presents the results of a series of experiments in which electrons are superelastically scattered from various laser excited states of sodium. The atoms, once in the optically prepared state, are forced to relax via the superelastic collision with an electron. The rate of detection of superelastically scattered electrons was measured as a function of the laser polarisation which enabled pseudo Stokes parameters to be determined. These pseudo Stokes parameters are functions of both optical pumping parameters and atomic collision parameters. The optical pumping parameters describe the laser-atom interaction and the atomic collision parameters describe the electron-atom collision process. Three different laser excitation mechanisms were used to optically pump the atoms into various excited states. The first of these used a single laser tuned to the 32S 112(F'=2 hyperfine state)-~32P312 transition. The excited atoms underwent a superelastic collision with an electron leaving the atom in the ground state and pseudo Stokes parameters were measured as a function of both scattering angle and incident electron energy. The second superelastic experiment, utilised a folded step excitation mechanism which employed two lasers tuned from the two hypethne states of the 32S112 ground state respectively to the 32P312 excited state. Power broadening effects in the single laser experiment cause the atoms to be optically pumped into the F= 1 hyperfine ground state. The laser powers used were not great enough to power broaden the hyperfine ground states and as such the F'= 1 sublevel effectively acted as a sink. The folded step excitation method enabled the excited state population to be increased so that data at larger scattering angles could be obtained. Stokes parameters from both of these experiments which had an incident energy range of 10eV to 30eV and an angular range of 5°-25° were compared to three current electron-atom scattering theories and previous experimental data. Overall, fair to good agreement was found between theory and experiments for the individual Stokes parameters. Losses of coherence was observed at small scattering angles (50.200) at 20eV and 25eV incident electron energies which were poorly modelled by the three different theories. The third superelastic experiment involved the use of two lasers of specified polarisation to stepwise excite the atoms to the 32D512 excited state. Superelastic collisions with incident electron energies of 20eV from the 32D512-*32P312~312 collision were studied at three different scattering angles and pseudo Stokes parameters for the case where the polarisations of the radiation from the lasers were parallel were measured. The single step and folded step laser-atom interactions for it excitation were modelled using a full quantum electrodynamical treatment so that the optical pumping parameters from the single and folded step experiments could be investigated. Equations of motion were derived in the Heisenberg picture and it is shown that for the single laser case 59 equations of motion are required to fully model the interaction and for the folded step ease 78 equations of motion are required. The results of calculations demonstrated that the optical pumping parameters were sensitive to laser intensity, laser detuning and the Doppler width of the atomic beam. The theoretical quantum electrodynamical calculation results were in good agreement with the experimental results.

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Arndt, Phillip Todd. "PROBING THE EXCITED ROVIBRATIONAL STATES OF SODIUM DIMERS". Miami University / OhioLINK, 2015. http://rave.ohiolink.edu/etdc/view?acc_num=miami1438641133.

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Scielzo, Nicholas David. "Measurement of the beta-neutrino correlation in laser trapped {sup 21}Na". Berkeley, Calif. : Oak Ridge, Tenn. : Lawrence Berkeley National Laboratory ; distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy, 2003. http://www.osti.gov/servlets/purl/821455-YDxgQ2/native/.

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Thesis (Ph.D.); Submitted to Univ. of California, Berkeley, CA (US); 1 Jun 2003.
Published through the Information Bridge: DOE Scientific and Technical Information. "LBNL--54350" Scielzo, Nicholas David. USDOE Director. Office of Science. Nuclear Physics (US) 06/01/2003. Report is also available in paper and microfiche from NTIS.

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Thomson, Robin Graham Crawford. "Laser spectroscopy of excited states in indium-mercury vapour mixtures". Thesis, Queen's University Belfast, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.334682.

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Weragoda, Geethika K. "Excited state intramolecular proton transfer (ESIPT) and trans-cis isomerization on the triplet excited states". University of Cincinnati / OhioLINK, 2015. http://rave.ohiolink.edu/etdc/view?acc_num=ucin1439296134.

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Chawla, Gunjit. "Study of long range potentials in excited states of diatomic sodium using modulated gain spectroscopy". Thesis, Massachusetts Institute of Technology, 1985. http://hdl.handle.net/1721.1/15297.

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Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Chemistry, 1985.
MICROFICHE COPY AVAILABLE IN ARCHIVES AND SCIENCE.
Includes bibliographical references.
by Gunjit Chawla.
Ph.D.

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Bohl, Elvira. "Investigating excited electronic states in fullerenes and polycyclic aromatic hydrocarbons using Femtosecond Laser Photoelectron spectrometry". Thesis, University of Edinburgh, 2016. http://hdl.handle.net/1842/25979.

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Fullerenes have highly excited electronic states with interesting properties for possible wide ranging applications including in electronics. These highly excited, Rydberg-like states, so-called superatom molecular orbitals (SAMOs), are diffuse low-angular momenta states with molecular orbitals centred on the hollow fullerene core. The SAMOs can be detected by femtosecond photoelectron spectroscopy (PES) and characterised by photoelectron angular distributions (PADs) combined with time-dependent density functional theory (TD-DFT) calculations. The photoelectron spectra of C60 and C70 show a peak structure below kinetic energies corresponding to the photon energy, superimposed on a thermal electron background. This peak structure was assigned to one-photon ionisation of the SAMO states based on PAD and TD-DFT. In this thesis, studies of the fullerene species C82 and Sc3N@C80 revealed PES and PAD with similar features to C60 and C70. The SAMO peaks became less prominent compared to the thermal electron background for increasing molecular size and decreasing symmetry, and were almost absent for the endohedral species. To provide more information about the influence of encapsulated atoms in the fullerene cage on the SAMO states, experiments on Li@C60 have been carried out. A lower thermal electron emission temperature and a splitting of the SAMO peaks has been observed for Li@C60 compared to C60. Nevertheless the binding energies are remarkably similar in all investigated fullerenes, which is important for any applications. Since the binding energies are about the same, but the ionisation potentials of the fullerenes are different, the excitation energy to the SAMOs scales with the ionisation energy. The reasons for the well-pronounced peak structure of the SAMO states in the PES of C60 could be explained by the similarity of the SAMOs to Rydberg states along with the higher photoionisation probabilities compared to valence states which were modelled by Benoît Mignolet and Françoise Remacle. As the SAMOs are highly excited electronic states, like Rydberg states, the potential energy surface of the neutral molecule and the ionised molecule are similar. Therefore the vibrational energy is conserved in the molecule during the photoionisation on the femtosecond time scale. The TD-DFT calculations on C60, carried out by Benoît Mignolet and Françoise Remacle, revealed the photoionisation probabilities of the SAMOs to be at least three orders of magnitude higher than for non-SAMOs for the applied experimental conditions. To test the prediction of the model, the relative photoionisation probabilities of the s-SAMO to p-SAMO and the s-SAMO to d-SAMO were obtained experimentally from the PES at various photon energies (2-3.5 eV) within this work. The analysis indicates remarkable agreement between the experiment and the theoretical values. Further quantum chemical calculations on a series of polycyclic aromatic hydrocarbons (PAHs) were carried out within this thesis, which revealed similar Rydberg-like molecular orbitals in analogy to the SAMOs in fullerenes. The first series included benzene, naphthalene, anthracene, tetracene, pentacene and hexacene. The second series consisted of phenanthrene, pyrene and coronene. Finally, the third series covered cubane, adamantane and dodecahedral C20. All modelled molecules showed diffuse, excited electronic states similar to the SAMOs. Within each series the binding energies of these states decrease with increasing molecular size as well as the ionisation energies, except for the 3rd series. A comparison between all series shows that the binding energies of the states for the 3rd series (the 3-D series) are slightly higher than for the 1st and 2nd series in relation to similar molecular size. The results of the coronene calculations are compared to experimental photoelectron spectra and are shown to be in good agreement with the experiments.

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Dickson, Nicole Marie. "Exploration of the Excited States of Organic Molecules and Metal Complexes Using Ultrafast Laser Spectroscopy". The Ohio State University, 2011. http://rave.ohiolink.edu/etdc/view?acc_num=osu1306872674.

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Zhang, Yunlong. "Ultrafast Time Resolved and Computational Studies of Diazo and Diazirine Excited States, and of Carbenes". The Ohio State University, 2010. http://rave.ohiolink.edu/etdc/view?acc_num=osu1267479070.

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Pant, Lok Raj. "The Radiative Lifetime Measurement on 61Σ+g (v = 9, 10, 11, J = 31) Excited States of Molecular Sodium Using Time Resolved High Resolution Doubled Resonance Spectroscopy". Miami University / OhioLINK, 2021. http://rave.ohiolink.edu/etdc/view?acc_num=miami1626966676896514.

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Części książek na temat "Laser excited states of sodium"

Muller, Harm Geert, i Marc Paul de Boer. "Population Trapping in Excited States". W Super-Intense Laser-Atom Physics, 279–86. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4615-7963-2_24.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-33 (Sodium)". W Supplement to I/25 A-F, 495. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_88.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-20 (Sodium)". W Supplement to I/25 A-F, 417–20. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_76.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-21 (Sodium)". W Supplement to I/25 A-F, 421–28. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_77.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-22 (Sodium)". W Supplement to I/25 A-F, 429–41. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_78.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-23 (Sodium)". W Supplement to I/25 A-F, 442–60. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_79.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-24 (Sodium)". W Supplement to I/25 A-F, 461–79. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_80.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-25 (Sodium)". W Supplement to I/25 A-F, 480–82. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_81.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-26 (Sodium)". W Supplement to I/25 A-F, 483–85. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_82.

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Sukhoruchkin, S. I., i Z. N. Soroko. "Excited Nuclear States for Na-27 (Sodium)". W Supplement to I/25 A-F, 486–88. Berlin, Heidelberg: Springer Berlin Heidelberg, 2016. http://dx.doi.org/10.1007/978-3-662-48875-1_83.

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Streszczenia konferencji na temat "Laser excited states of sodium"

Perebeinos, Vasili. "Excited States Decay in Carbon Nanotubes". W Laser Science. Washington, D.C.: OSA, 2008. http://dx.doi.org/10.1364/ls.2008.lwk2.

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Avouris, Phaedon. "Excited states and electroluminescence of carbon nanotubes". W Laser Science. Washington, D.C.: OSA, 2006. http://dx.doi.org/10.1364/ls.2006.ltul1.

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Vellante, A., L. J. Qin, F. Giammanco i E. Arimondo. "Three-photon ionization in laser-excited sodium beam". W AIP Conference Proceedings Volume 172. AIP, 1988. http://dx.doi.org/10.1063/1.37337.

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Jorgensen, Christian K. "Excited States Of Laser-Emitting Ions". W French-Israeli Workshop on Solid-State Lasers, redaktorzy Georges Boulon, Christian K. Jorgensen i Renata Reisfeld. SPIE, 1989. http://dx.doi.org/10.1117/12.981457.

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Turpin, Pierre-Yves, Laurent Chinsky i Peter Mojzes. "Excited states in porphyrin-DNA interactions". W Laser Spectroscopy of Biomolecules: 4th International Conference on Laser Applications in Life Sciences, redaktor Jouko E. Korppi-Tommola. SPIE, 1993. http://dx.doi.org/10.1117/12.146142.

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Leone, Stephen R. "Attosecond transient absorption of field-manipulated excited states". W Laser Science. Washington, D.C.: OSA, 2013. http://dx.doi.org/10.1364/ls.2013.lth2i.2.

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Sinitsa, Leonid N. "Intracavity laser spectroscopy of highly excited molecular states". W Intracavity Laser Spectroscopy, redaktorzy Eduard A. Sviridenkov i Leonid N. Sinitsa. SPIE, 1998. http://dx.doi.org/10.1117/12.302463.

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Tarana, M., i Chris H. Greene. "Femtosecond XUV transparency in light-coupled He doubly excited states." W Laser Science. Washington, D.C.: OSA, 2011. http://dx.doi.org/10.1364/ls.2011.lwc1.

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Kuik, G., R. van Leeuwen, R. de Graaf, W. Vassen, W. Ubachs i W. Hogervorst. "Laser spectroscopy of doubly-excited states in barium". W Thirteenth International conference on atomic physics (ICAP-13). AIP, 1993. http://dx.doi.org/10.1063/1.43784.

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Cheret, M., L. Chen, D. Porterat i G. Spiess. "Doubly-excited Ba states with a circular Rydberg electron". W The XIth International conference on laser spectroscopy. AIP, 1993. http://dx.doi.org/10.1063/1.45039.

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Raporty organizacyjne na temat "Laser excited states of sodium"

Tischer, H., i A. V. Phelps. Detection of Excited States by Laser-Induced Fluorescence. Fort Belvoir, VA: Defense Technical Information Center, kwiecień 1985. http://dx.doi.org/10.21236/ada155558.

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