Contains research objectives and reports on five research projects

Aubrey, B. B.

Edmonds, D. S., Jr.

Haun, R. D., Jr.

Holloway, J. H.

King, J. G.

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VIII. ATOMIC BEAM RESEARCHProf. J. R. Zacharias S. J. Buchsbaum C. L. SchwartzDr. J. G. King D. S. Edmonds, Jr. H. H. StrokeB. B. Aubrey R. D. Haun, Jr. R. WeissJ. H. HollowayRESEARCH OBJECTIVESThe present interests of the atomic beam laboratory are:1. To exploit the inherent high precision of the atomic beam method. Experi-mental work is being continued to utilize this accuracy in a primary frequency stand-ard. An apparatus which has a theoretical frequency precision of one part in 1012 isunder construction. Another possible application of this work is a better understandingof the hyperfine structure interaction.2. To investigate the structure of nuclei through a study of the static propertiesof their ground states. In particular, measurements of the spins, magnetic dipole, elec-tric quadrupole, and magnetic octupole interaction are being carried out on certainnuclei. Information concerning the distribution of nuclear magnetism is also obtainedfrom a study of the hyperfine structure anomaly in various isotopes, and some experi-mental work along these lines has been completed.A. ELECTRON MULTIPLIERSTo detect the beam of atoms in an atomic beam experiment, it is necessary to useeither an electron multiplier or an FP 54 electrometer tube. The multipliers used here-tofore consisted of 15 copper-beryllium plates with a difference of potential of 200 voltsbetween successive stages. However, because activated copper-beryllium becomes con-taminated when exposed to air for periods longer than about 4 hours, it was decided totry to replace the copper-beryllium with silver-magnesium, which, when activated, issupposed to remain uncontaminated even after exposure to air for long periods of time.Before using these silver-magnesium multipliers in an actual experiment it is necessaryto measure their efficiency and to study their operating characteristics. These meas-urements are being carried out.B. B. AubreyB. PRECISION MEASUREMENTS OF THE HYPERFINE LEVELS OF Cs 1 3 3This work is part of our current program of precision measurements in cesium. Itconsists of the remeasurement of the transitions between the levels into which the ground133electronic state of Cs is split by the action of both nuclear and external magneticfields. Higher precision than has previously been obtained is now available through theuse of better frequency sources for frequencies around 10, 000 Mc/sec and through theuse of Ramsey's method (1) of inducing transitions by the insertion of the radiofrequencyfield at two points, one at the beginning and one at the end of the transition region.The apparatus used in this experiment is well suited to this work because it has along homogeneous magnet (C-field) and hence makes available a long transition region.-31-(VIII. ATOMIC BEAM RESEARCH)Work has been centered on modifications of the vacuum system and construction of adirectional oven of a multichannel type. Both are now complete. The oven has beensuccessfully placed in operation. The system for inserting the required frequencies atthe two points at the ends of the transition region in the proper relative phase is beingdesigned.D. S. Edmonds, Jr.References1. N. F. Ramsey, Phys. Rev. 78, 695 (1950).C. STARK EFFECT ON HYPERFINE STRUCTUREThe cesium atomic frequency standard (see the Quarterly Progress Report, Oct. 15,1954, page 30) has been modified so that both beams of atoms can be observed simul-taneously. Provision has been made for the application of a strong dc electric field inthe observation region between the two Ramsey rf regions in the left beam. The otherbeam still operates as described in the Quarterly Progress Report, October 15, 1954(that is, as a frequency standard). By measuring the difference in resonance frequenciesfor the two beams as a function of the electric field, the Stark effect on hyperfinestructure will be measured. Although the main effect will arise from the atomic elec-trons, it is hoped that it may prove possible to obtain information regarding the inter-action of the nucleus with the external field. If the nuclear effect proves to be detectable,the experiment will provide an upper limit for the "induced" electric dipole moment ofthe nucleus and experimental knowledge of the degeneracy of the nuclear ground state.R. D. Haun, Jr.2D. STUDY OF THE HYPERFINE STRUCTURE OF THE P STATEIN Ga69 AND Ga 7 1This study will complete our program of analysis on the stable gallium isotopes.Our specific objective this time is the investigation of the Bohr-Weisskopf effect in the2Pl/2 state. Before the 2P1/2 state could be studied, a fairly complete overhaul of theexisting apparatus was necessary because of the magnetic deflecting fields and thetransition frequencies required. The redesign was completed and construction is inprogress.J. H. HollowayE. HYPERFINE STRUCTURE OF HALOGENSEquipment is being prepared to measure the hyperfine structure of the long-lived(107 years) iodine isotope 1129. A 5-mg sample of this isotope has been obtained from32-(VIII. ATOMIC BEAM RESEARCH)Oak Ridge. The development of the following items is under way:1. recirculating, directive, microwave-arc atom source;2. electron multipliers and mass spectrometers for high-resolution, negativeion detection;3. 10-cycle flop modulators and detectors;4. rf sources consisting of klystrons for preliminary measurements and cavity-triode oscillators for final measurements;5. automatic data recording (100 kc/sec/min, tentative speed) and frequencyindexing.Because of the smallness and rarity of the 1129 sample, a relatively large amountof time and thought is being devoted to apparatus details with the hope of making it possi-ble to obtain all the data within a few days, thus minimizing the risk of losing thesample.J. G. King-33-

Atomic Beam Research

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Atomic Beam Research

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