GB1055613A - Frequency stabilisation of gas masers - Google Patents
Frequency stabilisation of gas masersInfo
- Publication number
- GB1055613A GB1055613A GB3927664A GB3927664A GB1055613A GB 1055613 A GB1055613 A GB 1055613A GB 3927664 A GB3927664 A GB 3927664A GB 3927664 A GB3927664 A GB 3927664A GB 1055613 A GB1055613 A GB 1055613A
- Authority
- GB
- United Kingdom
- Prior art keywords
- reflectors
- laser
- frequency
- tilt
- input
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/13—Stabilisation of laser output parameters, e.g. frequency or amplitude
- H01S3/139—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the mutual position or the reflecting properties of the reflectors of the cavity, e.g. by controlling the cavity length
- H01S3/1398—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the mutual position or the reflecting properties of the reflectors of the cavity, e.g. by controlling the cavity length by using a supplementary modulation of the output
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/13—Stabilisation of laser output parameters, e.g. frequency or amplitude
- H01S3/131—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation
- H01S3/134—Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation in gas lasers
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Abstract
1, 055, 613. Photo-electric control of laser frequency. NIHON DENSHI KABUSHIKI KAISHA. Sept. 25, 1964, No. 39276/64. Heading G1A. [Also in Divisions H1 and H3] The frequency of a gaseous optical maser (laser) is stabilized by frequency modulating the resonance tuning of the laser and detecting the fundamental and harmonic components of the modulating frequency in the laser output, then feeding the detected outputs to vary the horizontal and vertical tilt angles of the reflectors (to maintain them parallel), and their distance apart, and also to keep constant the pumping input power and output of the laser. The reflectors 2a, 2b are mounted on end plates spaced by four invar rods carrying current input windings 6a-6d, 7a, 7d and 8c, 8d which when energized vary by magnetostriction, the tilt and separation apart of the reflectors. Modulating frequencies e.g. 70 c/s and 25 c/s are applied to certain of the windings and from the partially translucent reflector 2b the light output is detected and amplified by a photo-multiplier tube. The fundamental, second and third harmonics of the 70 c/s input, separated by narrow band amplifiers, respectively provide a measure of (1) pumping input power variation (2) tilt of the reflectors in one direction, and (3) separation of the reflectors; and after detection in phase sensitive rectifiers and amplifying, are then respectively applied as automatic gain control to the pumping source, and to control windings on the invar rods to correct reflector tilt in one plane, and separation of the reflectors. The other input, 25 c/s, similarly corrects tilt in a plane at right angles to the first. The laser is so controlled that the first, second and third derivatives of the input power are all zero. The discharge tube 1 (containing a neon and helium mixture) is supported between the mirrors 2a, 2b and end plates by bellows 4a, 4b. The frequency 75 c/s and its harmonics may be derived by frequency division from a 450 c/s source.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB3927664A GB1055613A (en) | 1964-09-25 | 1964-09-25 | Frequency stabilisation of gas masers |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB3927664A GB1055613A (en) | 1964-09-25 | 1964-09-25 | Frequency stabilisation of gas masers |
Publications (1)
Publication Number | Publication Date |
---|---|
GB1055613A true GB1055613A (en) | 1967-01-18 |
Family
ID=10408662
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB3927664A Expired GB1055613A (en) | 1964-09-25 | 1964-09-25 | Frequency stabilisation of gas masers |
Country Status (1)
Country | Link |
---|---|
GB (1) | GB1055613A (en) |
-
1964
- 1964-09-25 GB GB3927664A patent/GB1055613A/en not_active Expired
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