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1 Feb 1970

Volume 16, Issue 3, pp. 87-144

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ELECTRON TUNNELING INTO AMORPHOUS GERMANIUM

J. W. Osmun and H. Fritzsche

Appl. Phys. Lett. 16, 87 (1970); http://dx.doi.org/10.1063/1.1653131 (3 pages) | Cited 20 times

Online Publication Date: 21 October 2003

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Al☒Al2O3☒Ge tunnel junctions were prepared to study electron tunneling into amorphous germanium films. An almost symmetric conductance minimum centered at zero bias without additional structure was observed. The change in conductance from 1V to zero bias is 103 at 78°K and about 102 at 300°K. The zero bias conductance is 102 times lower at 78°K than at 300°K. The results indicate a large density of states in the gap or near the surface.

TRANSITIONS BETWEEN MODE‐LOCKED STATES IN INTRACAVITY PHASE‐MODULATED LASERS

D. L. Lyon and T. S. Kinsel

Appl. Phys. Lett. 16, 89 (1970); http://dx.doi.org/10.1063/1.1653132 (3 pages) | Cited 5 times

Online Publication Date: 21 October 2003

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The transition between the two possible pulse train outputs of a mode‐locked laser was studied. The experimental results are in close agreement with a simple, phenomenological model of the transition.

TECHNIQUE OF MAPPING ACOUSTIC FIELDS BY MEANS OF A POLAROID FILM

Keigo Iizuka

Appl. Phys. Lett. 16, 91 (1970); http://dx.doi.org/10.1063/1.1653133 (3 pages)

Online Publication Date: 21 October 2003

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A standard Polaroid film was proved to be applicable to a quick and easy direct mapping of an acoustic field. The method utilizes the effect of an acoustic field on the developing process of a uniformly pre‐exposed Polaroid film. The method would be most useful for visualization of acoustic field as well as preparing acoustic holograms.

DIRECT OBSERVATION OF A DYNAMIC BURSTEIN SHIFT IN A GaAs:Ge PLATELET LASER

P. D. Dapkus, N. Holonyak, R. D. Burnham, and D. L. Keune

Appl. Phys. Lett. 16, 93 (1970); http://dx.doi.org/10.1063/1.1653134 (3 pages) | Cited 17 times

Online Publication Date: 21 October 2003

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Data (77°K) are presented showing a dynamic Burstein shift of the absorption edge during spontaneous and laser operation of GaAs:Ge platelets. This is indicated directly by an increase in the relative transmission of the pump power through the sample with increased pump excitation. By the use of pumps with photon energies (1.527 eV) closely matched to the GaAs absorption edge (1. 513 eV), changes in the relative transmission of from 4 to 30% have been achieved. The data presented also show a change in the rate of decrease of the absorption with the onset of stimulated emission by the platelet.

SELF‐STABILIZATION AND NARROWING OF OPTICAL PULSES FROM GaAs JUNCTION LASERS BY INJECTION CURRENT FEEDBACK

Thomas L. Paoli and José E. Ripper

Appl. Phys. Lett. 16, 96 (1970); http://dx.doi.org/10.1063/1.1653135 (2 pages) | Cited 7 times

Online Publication Date: 21 October 2003

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Self‐induced intensity pulsations of continously operating GaAs junction lasers have been frequency‐stabilized and narrowed by regenerative feedback of oscillations in the injection current. The spectral width of the pulse rate has been reduced by a factor of 20 to less than 30 kHz while the optical pulse width was reduced by at least a factor of 2 to less than 180 psec. These results suggest that a well‐stabilized source of short optical pulses can be constructed from GaAs injection lasers without external microwave circuitry.

ON THE PROPAGATION OF HIGH‐CURRENT BEAMS OF RELATIVISTIC ELECTRONS IN GASES

M. L. Andrews, H. Davitian, D. A. Hammer, H. H. Fleischmann, J. A. Nation, and N. Rostoker

Appl. Phys. Lett. 16, 98 (1970); http://dx.doi.org/10.1063/1.1653136 (3 pages) | Cited 22 times

Online Publication Date: 21 October 2003

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The transit time of high current beams of relativistic electrons (40–50 kA, 350 keV) through an air filled (0.2–2.5 Torr) drift tube has been measured. It is longer than expected, even allowing for the loss of beam front electrons and for orbiting of the electrons in the beam self‐magnetic field. Also, a pressure‐dependent nonuniformity in the beam motion was observed which may account for this delay.

VACANCY CLUSTERS IN DISLOCATION‐FREE SILICON

A. J. R. de Kock

Appl. Phys. Lett. 16, 100 (1970); http://dx.doi.org/10.1063/1.1653111 (3 pages) | Cited 51 times

Online Publication Date: 21 October 2003

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Dislocation‐free silicon crystals made by the floating zone technique contain vacancy clusters formed during cooling of the crystal after growth. The distribution and concentration of these defects have been determined. A model is presented describing the formation of these clusters. The influence of vacancy clusters on the leakage current of planar diodes is investigated.

ION IMPLANTATION DEPTH DISTRIBUTIONS: ENERGY DEPOSITION INTO ATOMIC PROCESSES AND ION LOCATIONS

David K. Brice

Appl. Phys. Lett. 16, 103 (1970); http://dx.doi.org/10.1063/1.1653112 (4 pages) | Cited 31 times

Online Publication Date: 21 October 2003

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A useful method of calculating the energy∕unit depth deposited in atomic processes by energetic ions in solids is presented. The calculated energy density is shown to correlate well with previous Monte Carlo calculations of the vacancy concentration resulting from ion bombardment and recent experimental measurements of the depth distribution of ion damage. The method also provides the depth distribution of ions in the solid as a function of their energy during the stopping process. This information would allow, for example, calculation of the location and rate of various energy‐dependent interactions between incident ions and host atoms.

DEPTH DISTRIBUTION OF DIVACANCIES IN 400‐keV O+ ION‐IMPLANTED SILICON

H. J. Stein, F. L. Vook, and J. A. Borders

Appl. Phys. Lett. 16, 106 (1970); http://dx.doi.org/10.1063/1.1653113 (3 pages) | Cited 27 times

Online Publication Date: 21 October 2003

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The integral depth distribution for divacancies produced in silicon at room temperature by 400‐keV O+ion implantation has been measured. The divacancy distribution was determined from repeated measurements of the characteristic 1. 8μ absorption band following successive anodizations and strippings of the implanted layer. Most of the divacancies are located between 4500 and 12 000 Å with a half‐value at ∼ 7500 Å and a concentration of ∼ 4 × 1019 cm−3 near the center of the distribution. The measured integral depth distribution for the ion‐produced divacancies is proportional within experimental error to theoretical calculations by Brice for the integral depth distribution of ion energy spent in atomic processes.

DEPTH DISTRIBUTION OF EPR CENTERS IN 400‐keV O+ ION‐IMPLANTED SILICON

K. L. Brower, F. L. Vook, and J. A. Borders

Appl. Phys. Lett. 16, 108 (1970); http://dx.doi.org/10.1063/1.1653114 (3 pages) | Cited 21 times

Online Publication Date: 21 October 2003

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The depth distribution of Si‐P3 centers in 400‐keV O+ ion‐implanted silicon was determined using EPR measurements in conjunction with anodization and stripping of the implanted layer. The depth distribution of the EPR centers compares favorably to theoretical calculations by Brice for the depth distribution of the energy deposited into atomic processes and with infrared absorption measurements of the depth distribution of divacancies by Stein, Vook, and Borders. The combined EPR and infrared measurements indicate that the Fermi level in the damaged layer lies between Ec − 0.21 eV and Ev + 0.25 eV.

SPIN‐WAVE EXPERIMENTS: PARAMETRIC EXCITATION OF ACOUSTIC WAVES AND MODE‐LOCKING OF SPIN WAVES

S. Wang and Ta‐lin Hsu

Appl. Phys. Lett. 16, 111 (1970); http://dx.doi.org/10.1063/1.1653115 (3 pages) | Cited 3 times

Online Publication Date: 21 October 2003

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In a spin‐wave instability experiment, a YIG disk was bonded onto a quartz rod with a transducer attached to it, and was placed in a microwave cavity in a parallel‐pumping arrangement. For microwave power above the threshold for spin‐wave instability, parametric generation of acoustic waves was observed. The generation was evidenced by the simultaneous appearance of a low‐frequency oscillation in the reflected microwave power and at the transducer. In a subsequent experiment, a low‐frequency acoustic wave was sent into YIG through the transducer. A great enhancement of the oscillation in the reflected microwave power was observed. The enhancement was due to phase‐locking of spin‐wave modes.

LASER‐GENERATED STRESS WAVES

N. C. Anderholm

Appl. Phys. Lett. 16, 113 (1970); http://dx.doi.org/10.1063/1.1653116 (3 pages) | Cited 75 times

Online Publication Date: 21 October 2003

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A method of generating stress waves with a laser is demonstrated using a transparent material to impede the expansion of the vaporized absorber. A stress wave whose magnitude is 34 kbar and whose width at half‐maximum is equal to the width of the laser pulse is reported.

SHOT NOISE IN JOSEPHSON POINT CONTACTS

H. Kanter and F. L. Vernon

Appl. Phys. Lett. 16, 115 (1970); http://dx.doi.org/10.1063/1.1653117 (3 pages) | Cited 12 times

Online Publication Date: 21 October 2003

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Experimental evidence is presented showing that the noise in Josephson point contacts is shot noise limited. Comparison with theory indicates that the pair current contribution is not as large as predicted.

CARBON MONOXIDE CHEMICAL LASER UTILIZING A FAST FLOW SYSTEM

Curt Wittig, J. C. Hassler, and P. D. Coleman

Appl. Phys. Lett. 16, 117 (1970); http://dx.doi.org/10.1063/1.1653118 (2 pages) | Cited 24 times

Online Publication Date: 21 October 2003

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Lasing from chemically formed CO in the range 5.20–5.60 μ m has been observed in a fast flow (∼ 120 m∕sec) system. Atomic oxygen was formed in an O2☒He discharge and passed into the optical cavity where it reacted with CS2. The chemical reaction and excitation mechanism are discussed and compared to systems in which flash photolysis was used with CS2☒O2 mixtures. Power levels of the order of 0.1 W from an interaction region 10 mm i. d. ×30 cm long were obtained with an input energy of 3 J per pulse into the O2 dissociator.

SIMULTANEOUS OSCILLATION ON TWO ISOTOPIC LINES IN CO2 AND N2O LASERS

L. J. Schoen and A. M. Ronn

Appl. Phys. Lett. 16, 119 (1970); http://dx.doi.org/10.1063/1.1653119 (2 pages) | Cited 2 times

Online Publication Date: 21 October 2003

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The intensity of emission of a CO2 laser has been studied as a function of mole % of 13CO2. It was observed that over the range 1.1 to 56.1 mole % 13CO2 the integrated intensity did not change to within the ± 10 % accuracy of the measurement. Laser action switched from the 13C to the 12C species as a smooth function of mole % of the isotopic species; simultaneous oscillation of both systems was observed over a fairly wide concentration range. The intensity of an N2O laser was studied under identical conditions over the range 95 –1.1 mole % of 14N15NO. The integrated intensity was observed to oscillate erratically with varying percentage of 14N15NO. Laser action was not a smooth function of species concentration.

ULTRAFAST RISE TIME LASER‐INDUCED STRESS WAVES

P. S. Peercy, E. D. Jones, J. C. Bushnell, and G. W. Gobeli

Appl. Phys. Lett. 16, 120 (1970); http://dx.doi.org/10.1063/1.1653120 (3 pages) | Cited 16 times

Online Publication Date: 21 October 2003

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Stress pulses having rise times ≲1 nsec have been produced at the surfaces of solids. These were produced by the absorption of single laser pulses of time durations of ∼ 3 psec and energies up to 20 J.

NONRESONANT ABSORPTION OF ELECTROMAGNETIC WAVES IN A HIGH‐DENSITY PLASMA

G. Lisitano, M. Fontanesi, and E. Sindoni

Appl. Phys. Lett. 16, 122 (1970); http://dx.doi.org/10.1063/1.1653121 (3 pages) | Cited 56 times

Online Publication Date: 21 October 2003

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Efficient radio frequency (rf) heating of a high‐density plasma is obtained for any value of the containing magnetostatic field larger than that corresponding to electron cyclotron resonance.

SPONTANEOUS SINGLE‐FREQUENCY OUTPUT FROM A SPATIALLY HOMOGENEOUS Nd:YAG LASER

H. G. Danielmeyer and W. G. Nilsen

Appl. Phys. Lett. 16, 124 (1970); http://dx.doi.org/10.1063/1.1653122 (3 pages) | Cited 14 times

Online Publication Date: 21 October 2003

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By moving a Nd:YAG rod relative to the cavity field with velocities of the order of centimeters per second, we obtained single‐frequency oscillation close to the center of the gain curve with output powers up to 1.2 W. Our results can be understood quantitatively by considering the smoothing effect of the relative motion on the spatial distribution of the population inversion.

CHANNELING STUDY OF BORON‐IMPLANTED SILICON

J. C. North and W. M. Gibson

Appl. Phys. Lett. 16, 126 (1970); http://dx.doi.org/10.1063/1.1653123 (4 pages) | Cited 85 times

Online Publication Date: 21 October 2003

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The channeling technique has been used to determine the lattice location of boron implanted into silicon by using the B11 (p,α) nuclear reaction. Approximately 30% of the boron lies on substitutional sites after a room‐temperature implantation of 3×1015∕cm2. The substitutional content decreases with annealing temperature up to 700 °C and then increases at higher annealing temperature. This explains a reverse annealing behavior observed in the carrier concentration. Nearly all of the boron lies on substitutional sites after annealing at 1100 °C. The nonsubstitutional boron atoms do not occupy the normal tetrahedral interstitial sites. For annealing temperatures up to 500 °C they appear to lie along <110> atomic rows, but they do not lie midway between <110> row lattice sites. After higher‐temperature annealing their location appears less well‐defined.

ABSORPTION PROFILES AND INVERTED LAMB DIPS OF I2 VAPOR AT 633 nm AS STUDIED WITH A He☒Ne LASER

J. D. Knox and Yoh‐Han Pao

Appl. Phys. Lett. 16, 129 (1970); http://dx.doi.org/10.1063/1.1653124 (3 pages) | Cited 12 times

Online Publication Date: 21 October 2003

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The rotational‐vibrational structure of the B3Πog+X′Σou+ electronic transitions in I2127 and I2129 vapors have been examined in detail over a spectral range of 2000 MHz in the 633‐nm region using He3☒Ne20 and He3☒Ne22 lasers. In addition, the hyperfine components of the Lamb dips in these two vapors have been observed. Due to the increased absorption, the inverted Lamb dips are easily observed in I2129.

DIVACANCY MOTION ENERGY IN GOLD

J. J. Burton and D. Lazarus

Appl. Phys. Lett. 16, 131 (1970); http://dx.doi.org/10.1063/1.1653125 (2 pages) | Cited 1 time

Online Publication Date: 21 October 2003

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A new resistance measuring technique has been used to study the annealing of quenched gold. The technique gives continuous data and makes it possible to obtain both an instantaneous and an apparent annealing activation energy. The instantaneous activation energy is 0.52 ± 0.03 eV. This is identified as the motion energy of the divacancy in gold.

SPIN‐LONGITUDINAL AND SPIN‐SHEAR ELASTIC WAVE CONVERSION IN AN AXIALLY MAGNETIZED YIG ROD

F. R. Morgenthaler, S. M. Rezende, H. L. Hu, and A. Platzker

Appl. Phys. Lett. 16, 133 (1970); http://dx.doi.org/10.1063/1.1653126 (3 pages) | Cited 3 times

Online Publication Date: 21 October 2003

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We report the first successful conversion of z‐directed spin waves to longitudinal elastic waves (and vice versa) in an axially magnetized (z axis) single‐crystal YIG rod. The conversions — carried out at L‐band frequencies and room temperature — were possible because the symmetry axis of the rod was not along a principal crystallographic direction; the axis was chosen to be in a {100} plane at an angle of 22.5° with respect to a <100> direction in order to provide nearly maximum spin‐longitudinal elastic wave coupling.

HIGHER ELECTRIC FIELDS FOR STARK‐INDUCED INFRARED SPECTRA

W. J. Boyd, P. J. Brannon, and N. M. Gailar

Appl. Phys. Lett. 16, 135 (1970); http://dx.doi.org/10.1063/1.1653127 (3 pages) | Cited 5 times

Online Publication Date: 21 October 2003

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A Stark cell to study the normally inactive infrared spectrum of homonuclear diatomic molecules has been built. This cell utilizes parallel metal plates to apply high electric fields across the sample gas. Fields of 240 000 V∕cm in H2 and 350 000 V∕cm in N2 have been achieved at 400 psi using the new cell. The electric‐field‐induced pure rotation infrared spectra of H2 was observed. The frequencies of the S0(2), and S0(3) pure rotation lines were measured, and the molecular constants B0, D0, and H2 were calculated from these data.

SHORT‐RANGE ORDER IN AMORPHOUS GeTe FILMS

D. B. Dove, M. B. Heritage, K. L. Chopra, and S. K. Bahl

Appl. Phys. Lett. 16, 138 (1970); http://dx.doi.org/10.1063/1.1653128 (3 pages) | Cited 23 times

Online Publication Date: 21 October 2003

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Thin films of amorphous (stoichiometric) GeTe have been examined by direct recording of electron diffraction, and intensity profiles across the diffuse diffraction pattern have been recorded with electrostatic rejection of inelastically scattered electrons. Radial distribution analysis of these curves shows that the local order is not characteristic of the distorted rocksalt structure of bulk GeTe, i.e., nearest‐neighbor distance of 2.99 Å and nearest‐neighbor coordination of 6. Instead it is found that the nearest‐neighbor distance is 2.65 Å with coordination of approximately 4. This result is of significance for the interpretation of the electronic properties of amorphous films.

HIGH‐SPEED SPECTROSCOPY USING THE INVERSE RAMAN EFFECT

R. A. McLaren and B. P. Stoicheff

Appl. Phys. Lett. 16, 140 (1970); http://dx.doi.org/10.1063/1.1653129 (3 pages) | Cited 14 times

Online Publication Date: 21 October 2003

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A method of obtaining inverse Raman spectra over the range of frequency shifts ∼ 300–3500 cm−1 in liquids and solids in a time of ∼ 40 nsec is described. The stimulating monochromatic radiation at 6940 Å is provided by a giant‐pulse ruby laser; the background continuum is the short‐lived spontaneous fluorescence of rhodamine B or 6G excited by second‐harmonic radiation (3470 Å) produced in KDP from a small part of the main laser beam, thus ensuring simultaneous irradiation of the sample by both beams.
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