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Time and Frequency Division

Technical Highlights

  • Deterministic Quantum Entanglement. Q. Turchette, C. Monroe, D. Wineland, and other members of the quantum computer project of the Ion Storage Group have recently demonstrated the ability to entangle two quantum particles with high efficiency, advancing the possibilities for reducing noise in stored-ion frequency standards and demonstrating realistic quantum computation. Previously, entanglement of particle states was obtained by post selection from a large number of trial experiments, such as the production of two correlated photons that occasionally occurs when a single photon passes through a special crystal. Such entanglement has proven useful for tests of quantum nonlocality, but entangling a large number of quantum particles--essential for noise reduction in atomic frequency standards and for building a practical quantum computer--becomes much less likely if it is dependent on a probabilistic process. In their "deterministic entanglement" process, a pair of beryllium ions is confined in an ion trap and laser cooled. Using a predetermined sequence of laser pulses, the internal spin of one ion is entangled with the ions' shared external motion, and the motion is entangled with the spin of the other atom. Entangled spins are therefore obtained "on demand" in each trial. It should be possible to apply the techniques used in these experiments to entangle larger numbers of ions. (Q. Turchette)
  • Lithographically Fabricated Micro-Traps. In collaboration with J. Beall of EEEL, C. Myatt of the Ion Storage Group has designed and fabricated the first-generation, lithographic, linear ion trap from a ceramic substrate with gold-plated electrodes. Lithographic fabrication (see Fig. 1) provides for more precise control of dimensions for small traps, and allows construction of the much-more-complex trap arrangements needed for future work on the entanglement of larger numbers of ions.

    Figure 1

    Figure 1. Schematic representation of the lithographic trap. The four rods in the traditional linear trap are shown at the top. In the new trap, shown with substantial separation between the two substrates for clarity, metallization along edges of the slots in the two substrates replaces the rods.
    Small numbers of ions have been laser cooled and crystallized in the trap with confinement provided by alternating electric fields at frequencies up to 200 MHz. Independent laser beams have been tightly focussed on each of the two trapped ions, which were separated by about 5 µm, with the off-focus ion receiving only 1/5 of the radiation intensity intended for the other ion. This is important because many of the applications of these entangled states require the separate addressing of individual ions. In addition, the Group has recently shuttled ions along the axis of the trap and separated them by applying pulsed voltages to the electrodes. This technique may relax the laser-focusing constraints for quantum logic gates and individual ion detection and suggests the possibility of multiplexing a more complex array of trapped ions by moving ions between accumulators. (C. Myatt)
  • Laser Cooling to the Ground State for Two Ions B. King and other members of the quantum computer project of the Ion Storage Group have cooled two ions to the ground state of motion, an important step in reducing noise in stored-ion frequency standards and in implementing quantum logic operations on multiple ions. Of critical importance is the heating rate and decoherence of the modes of two-ion motion. The Group found that the center-of-mass modes of the ion pair are heated at a rate of 5 quanta/ms to 10 quanta/ms, similar to previous single-ion results. However, the three, internal, motional modes (stretch and rocking modes) are found not to suffer from heating, up to the level of experimental uncertainty of about 0.1 quanta/ms. This is not unexpected, since the internal modes are immune from the effects of noisy fields affecting both ions equally. The heating results indicate that the (unknown) source is not differential heating, thus ruling out sources such as atomic collisions, field gradients, and certain types of rf-micromotion heating.

    These results imply that internal modes are more suitable than any center-of-mass mode for use in quantum-logic or noise-reduction schemes following the general proposal of Cirac and Zoller. However, any logic operation will be affected to higher order by motion in at least one of the center-of-mass modes, so center-of-mass heating remains a concern. (B. King)
  • Narrowest Linewidth Laser. In the course of recent efforts to develop an optical frequency standard, B. Young and J. Bergquist, with F. Cruz from Brazil, have demonstrated the narrowest-linewidth visible laser ever built. The ultimate goal of this project is to lock a narrow-linewidth laser to a well defined (282 nm, 2 Hz linewidth) transition in 199Hg+ ions. The resulting optical frequency standard could be used directly in the optical region, or frequency divided to the microwave region to serve as a traditional atomic clock.

    In order to demonstrate the performance of the new laser system, the difference frequency (beatnote) between two laser beams, locked to independent reference cavities on independent isolation platforms, was shown to have a linewidth of 0.84 Hz for an averaging time of 40 s (see Fig. 2). This implies that the linewidth of one of the lasers was less than 0.6 Hz, corresponding to a fractional linewidth of about 1 × 10-15. The key to this result is the isolation from seismic and acoustic noise and from pressure and temperature fluctuations of the high-finesse, optical cavities used to stabilize the lasers.

    Figure 2

    Figure 2. Beatnote observed in mixing the outputs of two separate 563 nm sources. The inset shows the simple experimental arrangement. The data are for a measurement time of 40 s.
    The performance of this laser is now better than that needed for a local oscillator for the optical, mercury-ion, frequency standard. Since systematic frequency shifts for the optical-frequency standard are anticipated to be very small, this new standard should perform better than all previous frequency standards. (J. Bergquist)
  • A Diode-Laser, Optical Frequency Standard Using Trapped Calcium Atoms. C. Oates, L. Hollberg, and guest researcher F. Bondu have developed and tested an all-diode-laser optical frequency standard based on trapped, laser-cooled, calcium atoms. Measurements of the intercombination line at 657 nm demonstrate linewidths as narrow as 400 Hz (line Q = 1012), the natural linewidth for this transition. The fractional frequency stability of a laser locked to this resonance (in an unoptimized system) is already 5 × 10-14 τ-1/2, where τ is the averaging time. Ramsey fringes for typical operating conditions are shown in Fig. 3. The narrow linewidth of the transition along with the convenient wavelengths for probing and cooling (allowing use of diode lasers for interrogation and cooling) makes this an especially attractive optical-frequency standard.

    Figure 3

    Figure 3. Ramsey fringes for the cold-calcium optical frequency standard.

    The trapping and cooling light at 423 nm is generated by frequency doubling 846 nm light from a semiconductor master-oscillator power amplifier. This provides 50 mW of 423 nm light, which is used to cool and trap 107 atoms in 20 ms. A "shelving-detection" scheme, similar to that used for spectroscopy of trapped ions, has been used to interrogate the calcium line and stabilize the frequency of the 657 nm laser (fast linewidth of about 50 Hz). A phase-coherent, frequency-measurement chain for connecting this transition to the 282 nm transition of the mercury ion is now under development. (C. Oates).
  • Subsystems for Optical Frequency Measurements. Staff members of several Groups in the Division have developed laser-frequency measurement technologies for application to the construction of a frequency synthesis system capable of measuring optical frequencies with an accuracy limited by atomic frequency standards. The system will be used to interconnect and compare new optical-frequency standards such as the calcium and mercury-ion standards, and eventually to connect these references to the cesium primary frequency standard. The design concept involves three successive subdivisions of optical-frequency intervals plus one frequency doubling to arrive at a point at which ultrashort laser pulses can be used to measure the smallest frequency interval relative to the cesium primary standard. The ultrashort-pulse technique (developed at the Max Planck Institute) to be used in this last step involves a comb of closely spaced frequencies generated by a mode-locked, titanium-sapphire laser.

    The larger steps of optical-frequency subdivision are achieved using mixing crystals of periodically poled lithium niobate. These crystals have been custom fabricated (in collaboration with staff of EEEL) to obtain efficient second-harmonic generation and sum/ difference frequency generation. With these devices a preliminary measurement was made of the mercury ion transition (532.360 800 THz) relative to the accurately known calcium transition at 657 nm. Further development of the system this year will provide an improved measurement of the mercury-ion transition relative to the calcium transition. Completion of the connection to the cesium standard is expected within approximately two years. (L. Hollberg and J. Bergquist)
  • Direct Observations of Spatial Structure of Crystallized Ion Plasmas. Large numbers of beryllium ions (up to 106 or more) can be stored in Penning traps by a combination of static electric and magnetic fields and laser-cooled temperatures so low that the ions freeze into a rigid lattice. Previously, Bragg scattering with the same laser light used to cool the ions was used to determine general features of the spatial structure. It was found that, for approximately spherical plasmas having 200,000 or more ions, the Bragg scattering pattern was consistent with a body-centered cubic (bcc) lattice, the theoretically predicted structure for the infinite-volume limit.

    More recently, T. Mitchell, J. Bollinger, and W. Itano of the Division observed direct images of the ions fluorescing in large, spherical plasmas. These images showed the central regions of the plasmas to have bcc structure, or, more rarely, face-centered-cubic structure. In order to obtain these images, it was necessary to phase-lock the rotation of the plasma to an external electric field. The imaging camera could then be gated synchronously with the rotation, which has a frequency of about 1 MHz in this case. The ability to control the state of the plasma with this high a degree of accuracy would be of great importance to a frequency standard based on ions in a Penning trap.

    Very flat, radially extended plasmas have been observed to have a structure like a stack of planes. As the density of the ions is increased, the plasma goes through a series of structures having square, rhombic, or hexagonal ordering within a plane. At certain values of the density, another plane is formed. The observed structures are in good agreement with calculations made by D.H.E. Dubin of the U. California, San Diego. (W. Itano)
  • NIST-F1: A Cesium-Fountain Primary Frequency Standard. Over the last half year, S. Jefferts, D. Meekhof, and D. Lee, along with F. Levi of the IEN in Italy, have brought NIST's new cesium-fountain frequency standard into operation, and they recently completed a preliminary evaluation of its uncertainty at a level commensurate with that of NIST-7 (5 × 10-15). This evaluation was limited entirely by statistical noise (not systematic effects), since the stability of the standard is still more than an order of magnitude worse than we expected. A Ramsey pattern for the standard is shown in Fig. 4. The narrowest Ramsey fringe observed to date has a width of about 0.6 Hz. The magnetic field applied to separate the Zeeman lines is 0.1 µT, and the Ramsey fringes observed on the first Zeeman line indicate that the field along the flight path of the atoms is uniform to about 10 pT. This indicates that the magnetic shielding is quite good.

    This standard differs from other fountain standards in that the microwave cavity and atom drift tube are an integrated structure that serve as the vacuum chamber for the standard. This provides exceptional immunity to microwave leakage fields. For all other fountain standards, the microwave cavity and drift tube are contained within a vacuum chamber, and microwave leakage can cause difficulty. The laser system used to generate the multiple beams that cool, trap and launch the atoms involves a single master-oscillator power amplifier that provides sufficient power for all of the beams. Other fountain standards typically employ an array of independent diode lasers that are injection locked to a lower-power master oscillator. Future efforts on this project will focus on improving stability so that better evaluations can be made of systematic frequency shifts. (D. Meekhof and S. Jefferts)   Figure 4

    Figure 4. Ramsey fringes for the NIST cesium-fountain frequency standard. The dots show the actual data, while the lines simply connect data points in sequence, so the amplitude noise apparent in the envelope of the curve is not real.
  • A Laser-Cooled Primary Frequency Standard in Space. Several Groups within the Division, in collaboration with staff members of the Atomic Physics Division and a faculty member at the U. Colorado, are now engaged in a flight definition study for a laser-cooled-cesium clock in space. The project, called Primary Atomic Reference Clock in Space (PARCS), is aimed at an improved realization of the definition of the second, improved coordination of time/frequency standards on earth, and tests of several aspects of special and general relativity. The microgravity environment of space allows us to use slower atoms and increase interrogation time, thus improving clock performance. Assuming that the project can remain on an ambitious development schedule, flight should occur aboard the International Space Station (ISS) in 2003.

    Figure 5 shows a schematic diagram of the proposed clock. The core of the clock (the physics package) is made up of: 1) the atom-preparation region where atoms are laser cooled, trapped, and launched; 2) a microwave cavity where atoms are subjected to microwave radiation at the cesium resonance frequency; and 3) a detection region where laser fluorescence is used to determine whether the microwaves have caused a transition. The objective is to achieve a stability of 3 × 10-14 τ-1/2 and an absolute uncertainty of 1 × 10-16. (D. Sullivan)
  • Figure 5

    Figure 5. Diagram of the proposed space clock. Details of the microwave cavity have been omitted to more clearly show the expansion of the atom balls as they proceed through the cavity.

  • Joint U.S.-Japan Development of a Frequency Standard. A joint project between the Time and Frequency Division and the Communications Research Laboratory (CRL) in Japan to develop an improved version of NIST-7, the U.S. primary frequency standard, has recently been completed. The objectives of this project, funded by CRL, were to construct an optically pumped standard with an uncertainty comparable to that of NIST-7, to compare this new standard with NIST-7, and to improve a number of subsystems allowing for more-rapid, automated evaluation of systematic frequency offsets. B. Drullinger and D. Lee led the project, with major contributions from D. Jennings, L. Mullen, C. Nelson, J. Shirley and F. Walls. In addition, during the entire three-year course of development, at least one staff member from CRL was always engaged in the project.

    The final comparisons between the new standard and NIST-7 indicate agreement within the nominal uncertainty (5 × 10-15) of the two standards. Major improvements made during the project included a more robust diode-laser system for optical-state preparation and detection, new servo-control and monitor software using a more-flexible object-oriented approach, identification of a number of smaller sources of systematic offset, and improved modeling of several of the larger systematic frequency shifts. Improvements made to the new standard during this development project will now be incorporated in NIST-7. Aside from these improvements, the key benefit of this project was the demonstration of agreement between these independent standards. It would have been difficult for NIST to justify construction of a second standard for this purpose. (R. Drullinger)
  • Frequency Synthesizer for Laser-Cooled Atomic Clocks. F. Walls, with guest researchers A.S. Gupta and D. Popovic, has recently developed an improved microwave frequency synthesizer with a performance sufficient to support laser-cooled atomic clocks being developed as new primary frequency standards and for advanced space applications. This new synthesizer makes use of simple and rugged digital technology, some key components of which are already space qualified. The phase stability, temperature coefficient, and frequency agility should be more than adequate for every standard now under active development and might well serve generations of standards beyond these. It should also find application in standards for phase-noise and amplitude-noise measurements.

    The key design advances have been the use of digital technology and the removal of narrow-band filters, which typically produce temperature-stability and phase-stability problems. Measurements between a pair of these synthesizers are shown in Fig. 6. For each of the pair of synthesizers, these data indicate a fractional-frequency stability of better than 7 × 10-16 at 10 s, averaging down to 1 × 10-18 at 1 day. The measured temperature coefficient is 0.12 ps/K. This synthesizer is small, and the circuitry is easier and less costly to assemble since there are many fewer critical adjustments involved. (F. Walls)   Figure 6

    Figure 6. Measured fractional-frequency stability between two of the new microwave frequency synthesizers as a function of averaging time τ.
  • Improved Time-Scale Reference for Division Programs. T. Parker, F. Walls, and J. Levine have collaborated to improve both the performance of the NIST time scale and distribution of time-scale signals to key programs within the Division. Drift and noise in signal distribution to clock research laboratories and time-transfer stations have been reduced through installation of improved distribution amplifiers and much higher-quality coaxial cables. This has been needed particularly for studying and evaluating the new generation of laser-cooled frequency standards and for improving the reference used at satellite time comparison stations where the NIST time scale is compared with those of other world standards laboratories. The temperature coefficient of delay of the new cable is dramatically better than conventional cable, resulting in a more stable transmission delay despite the fact that the cable runs through areas that experience rather large temperature excursions.

    The real-time output of the time scale is now generated by steering the output of a special synthesizer (driven by a good clock in the time scale) to the ensemble average of the clocks in the time scale. Of course, steering corrections to international UTC are also interjected into this system. The RMS error in this generation is now below 10 ps, an improvement of about a factor of 30. Finally, all five of the NIST masers are now contributing to the time scale. This has improved the time-scale stability to σy(τ) · 3 × 10-16 at τ = 5 days. (T. Parker)
  • GPS Carrier-Phase Time Transfer. In collaborative work between J. Levine of the Division and K. Larson of the University of Colorado, GPS signals were used to achieve a time transfer resolution between Washington and Boulder of 100 ps for an averaging time of 1 day. The traditional approach to high-accuracy GPS time transfer involves two observers making observations of the same code-based timing signal from a satellite that can be viewed simultaneously by both. This approach is limited in resolution to 2 ns to 3 ns when averaging for 1 day.

    The method employed in these experiments uses the phase of the GPS microwave carrier (rather than the code) for the common-view time transfer. This process involves identifying the same cycle of the carrier (or cycles of the carrier separated by a constant number of cycles). This is a substantial problem because the frequency is high, each satellite is in common-view for only a short period, and there is no reference available to help identify a particular cycle. The process employed is patterned after that used by geodesists, wherein the observations from a large number of other sites are compared and adjusted to obtain consistency and arrive at the appropriate cycle identification. They were able to achieve this for periods lasting many weeks.

    This work is critical to the comparison of the frequency accuracy of new generations of laser-cooled, atomic frequency standards that are now being developed at laboratories around the world. The method should provide for an order-of-magnitude improvement in the precision of frequency comparison. This first experiment already allows frequency comparisons at a level of 1 × 10-15 over about 1 day. (J. Levine)
  • GPS Common-View Timing Receiver with Multiple Channels. J. Levine, V. Zhang, and A. Gifford have developed a Common-View Timing Receiver based on a commercially available, general-purpose, multi-channel GPS receiver. The system functionality is similar to that of earlier receivers developed at NIST except that the current receivers are much simpler and less expensive and track up to eight satellites simultaneously. One objective of this development was the replacement of older, NIST-developed receivers that have been used for many years for international time coordination. Many parts for these older receivers are no longer available, so maintenance is becoming progressively more difficult. Aside from Boulder, the new receivers are now located at the US Naval Observatory and the BIPM. Data from these receivers are automatically transmitted to NIST once each day.

    The receivers are also being used in other applications. For example, data from one receiver located at NIST are downloaded every morning to a web site providing the means for achieving NIST traceability using GPS signals. These receivers are also being installed at a number of DOD sites where they will be used to achieve high-level synchronization for DOD programs. (J. Levine)
  • Multipath Effects in Time Transfer. Improved primary frequency standards and time scales have put increasing demands on the performance of international time comparisons using GPS common-view and two-way time transfer. In an effort to respond to this demand, F. Ascarrunz and T. Parker have been studying methods for improving the performance of Division time-transfer systems. Of particular significance is their development of an understanding of the impact of multipath signals on time transfer with pseudo-random-phase codes used with both two-way satellite time transfer and with common-view, GPS time transfer. Their analysis shows that multipath effects exacerbate the difference between the observed phase delay and the group delay. This understanding should allow improvement of two-way time transfer through more appropriate choice of the code chip rate. It focuses more attention on minimizing multipath effects in common-view time transfer, where it is not feasible to make chip-rate changes.

    They have also developed a calibration system for two-way time transfer, providing a means for evaluating (and thus controlling) the delays through the entire satellite ground station. Improved cables have cut the delay variations in the calibration system from 200 ps to 50 ps. (T. Parker)
  • Frequency Traceability to NIST Using GPS. M. Lombardi and J. Levine have developed an on-line database of comparisons between the NIST time scale and the Global Positioning System (GPS) satellite signals. Calibration laboratories using GPS signals as a frequency reference can access the database to complete their chain of traceability to NIST. The database is automatically updated each morning and past data are archived. The archive allows users to retrieve past data and retroactively confirm the traceability of their measurements. This service was developed in response to requests from calibration and standards laboratories and from GPS receiver manufacturers who develop products for the time and frequency marketplace. (M. Lombardi).
  • Year 2000 Time/Date Service. The Time and Frequency Division has established a time server to assist users in testing the performance of time-setting software after the year 2000 (Y2K). The transmitted time of day is correct and is directly traceable to the NIST time scale, but the date portion of the message is exactly 2 years in the future. Access to the Y2K service is by telephone or through the Internet. All of the common digital time formats are supported.

    The service, developed by J. Levine was inaugurated at the end of October 1998, and will stay in operation through the end of 1999. To facilitate using the Internet-based test system, NIST has also modified its client software to allow users to select either the normal servers or this special test system. This modified software is available on the Internet. (J. Levine)
  • Completion of the Second Phase of Upgrade of WWVB. Staff members at the NIST radio-station site north of Fort Collins, Colorado, working with staff members of the Time and Frequency Group, have completed the second phase of upgrade of WWVB. This phase of upgrade of the 60 kHz broadcast service involved development of a second, identical, transmitting system including a reconditioned low-frequency antenna and associated helix house, new transmission line, and high-power transmitter. The two transmitting systems, operated together in phase, will produce 50 kW of radiated power. This should be compared with the initial starting point of 10 kW and the most recent output of 23 kW achieved following completion of the first phase of the upgrade. In emergencies, one transmitting system can radiate the full 50 kW of power. However, this mode of operation reduces tube life significantly. Modifications of the WWVB building, now in progress, will allow the installation of a third transmitter to back up the present transmitters. At 50 kW of radiated power, the broadcasts will more completely cover the continental United States as shown by the modeled, field-intensity contour in Fig. 7. This should allow for commercial development of a broader range of simple clocks and frequency standards based on these broadcast signals. (W. Hanson).
  Figure 7

Figure 7. Electric-field-intensity contours (100 µV/m) projected for operation of WWVB at 50 kW radiated power during night-time hours. The nulls in the pattern are caused by interference of the ground wave and the sky (reflected).
  • Lasers for Wavelength-Scanned Interferometry. R. Fox and L. Hollberg of the Division have been collaborating with L. Howard and J. Stone of the Precision Engineering Division of MEL on the development of rapidly scanned diode lasers for application to wavelength-scanned interferometry. This is a length-measurement process that does not require physical movement of the arm of an interferometer. The requirements for the laser system are that it must operate with a single longitudinal and transverse mode, and that its wavelength (oscillation frequency) can be scanned continuously and rapidly without mode jumps. After some study of several laser types, a distributed-Bragg-reflector laser with a three-electrode structure was selected for testing. The 852 nm laser and optics have been enclosed in a "hand-held," 40 × 40 × 100 mm package (see Fig. 8).

    Figure 8 Figure 8. Photograph of the new diode-laser source for wavelength-scanned interferometry.   A tuning range as broad as 1.3 nm at 852 nm was demonstrated, with the period for tuning through the full range being as short as a few ms. The modular electronic systems used to power and control the laser are of a standard design that could be substantially miniaturized if necessary. Staff members of the Precision Engineering Division are now testing the system. The objective of this joint project is to achieve precision length metrology with systems that can be easily used in a machine-shop environment. (R. Fox).

  • Optical Gain Without Population Inversion. In recent experiments conducted by J. Kitching and L. Hollberg, optical gain without population inversion (GWI) was observed in a sample of laser-cooled, trapped atoms. This gain results from quantum interference arising from coherences established in the atom by the applied optical fields. Interpretation of results on GWI and lasing without population inversion (LWI) has involved substantial controversy, and this experimental work stands out as particularly unambiguous in interpretation. In the experiments, 87Rb atoms were laser cooled and trapped in a magneto-optical trap (MOT). The observed gain was as much as 0.2% per pass through the trapped atoms at a wavelength of 795 nm in the presence of a strong drive laser at 780 nm. Direct measurements established that there was no population inversion between the relevant excited and ground states. Other measurements were made to rule out any explanation based on direct Raman processes. The results indicate promise for the use of optical coherences in generating shorter wavelength radiation. (L. Hollberg)
  • Compact Rubidium Oscillator. L. Hollberg and F. Walls, with guest researchers N. Vukievi and A. Zibrov, have developed a new frequency reference based on Raman transitions in rubidium. The objective is a frequency reference that is very compact, portable, and low-power. While several different modes of operation have been studied, the most promising involves the 3 GHz transition in 85Rb, where resonance linewidths as narrow as 800 Hz have been observed. This is an attractive transition because it permits the use of commercially available low-power electronics. The observed stability of a table-top prototype device, even in this embryonic stage of development, is < 1 × 10-10 between 1 s and 1000 s. Further development should result in a much better stability. With some engineering effort, the size of the device could be reduced to about 3 × 3 × 9 cm3 and the power consumption reduced to the order of 1 W. Studies of longer-term stability and environmental sensitivity are now underway. This oscillator has potential applications for electronic instrumentation, telecommunications, and aerospace systems. (L. Hollberg)
  • Nitrous-Oxide Frequency Standards. In measurements performed by K. Evenson and guest researchers T. Varberg and F. Stroh, substantial improvements have been made in the frequency uncertainties of more than 200 spectral lines of 14NO and 15NO covering the spectral range from about 200 GHz to 5 THz. Uncertainties for all of the measurements were 10 kHz or less. The measurements were made using tunable-far-infrared spectroscopy, wherein a tunable microwave signal is mixed with CO2 difference frequencies to produce probe radiation covering the desired spectral region. These laboratory measurements are needed for study of the ozone chemistry of the upper atmosphere and for calibration of Fourier-transform spectrometers. (K. Evenson).
  • Study of Bending Transitions in the Far Infrared. M. Allen and K.M. Evenson have collaborated with guest researcher H. Körsgen on the first high-resolution measurements of bending transitions in the far-infrared region of the spectrum. Laser-magnetic-resonance (LMR) spectroscopy was used to study these transitions in FeD2, CCN, HCCN and DCCN in the vicinity of 6 THz. The measurements were made possible by substantial improvements in the low-frequency output of the CO2-pumped methanol laser. Aside from providing accurate frequency references for radio astronomy searches for these molecules in the interstellar medium, the results should allow exacting tests of molecular theory for these molecules. (K. Evenson)
  • NIST Time Web Site Lauded for Educational Impact. The Time and Frequency Division's web site entitled "A Walk Through Time" was selected by the Tech Museum of Innovation as "one of the ten best technology web sites we've found for middle-school and above students, teachers, and parents" for the month of June, 1998. The "Tech Ten" award is presented to web sites that bring the best in technology education to middle-school and above audiences. To receive the award, web sites must be "focused on high technology and innovation; be relevant and understandable to a middle-school audience; and be fun and engaging."

    San Jose's Tech Museum of Innovation, in the heart of Silicon Valley, is a hands-on technology museum "devoted to inspiring the innovator in everyone." In citing the Time and Frequency web site, the museum noted "this history of time and measurement is anything but dry. Explore the mysteries of Stonehenge, or the calendars of ancient Babylon, all the way up through today's atomic clocks and satellite-broadcast time services. Time definitely doesn't stand still here." (J. Wessels)

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