JPS5617091A - Laser time standerdization device - Google Patents
Laser time standerdization deviceInfo
- Publication number
- JPS5617091A JPS5617091A JP9307879A JP9307879A JPS5617091A JP S5617091 A JPS5617091 A JP S5617091A JP 9307879 A JP9307879 A JP 9307879A JP 9307879 A JP9307879 A JP 9307879A JP S5617091 A JPS5617091 A JP S5617091A
- Authority
- JP
- Japan
- Prior art keywords
- laser beam
- frequency
- cell
- time signal
- molecule
- 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.)
- Pending
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
Abstract
PURPOSE:To obtain a highly precise standard time signal by making a laser beam emitted from a laser beam source devided into two equal parts and projected to an absorbing cell giving a reverse direction with each other and by performing a low frequency moduration for the laser beam in a way that the absorption center frequency of the molecule in the cell and the oscillation frequency of the beam source will be in coincidence with each other. CONSTITUTION:A laser beam from a laser beam source 10 is transmitted through a beam splitter 12 by reflecting it with a reflecting mirror 11 and the beam is devided into two making the beam intensity of one of them stronger than that of the other. Then, these beams are reflected with reflecting mirrors 13 and 14, giving a reversed direction with each other, and projected into an absorption cell 15, wherein a molecule presenting Hall burning phenomenon is sealed, and the laser beam emitted from the above is detected by a detector 16. Subsequently, the detected beam is controlled by a tuning control circuit 17, a low frequency modulation is performed for the beam frequency, being fed back to a beam source 10 and is coincided with the absorption center frequency of the molecule in the cell 15. Then, said coincided frequency is emitted as a standard time signal through a standard time signal generating circuit.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9307879A JPS5617091A (en) | 1979-07-20 | 1979-07-20 | Laser time standerdization device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9307879A JPS5617091A (en) | 1979-07-20 | 1979-07-20 | Laser time standerdization device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5617091A true JPS5617091A (en) | 1981-02-18 |
Family
ID=14072473
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9307879A Pending JPS5617091A (en) | 1979-07-20 | 1979-07-20 | Laser time standerdization device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5617091A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0468738U (en) * | 1990-10-29 | 1992-06-18 | ||
JPH06334253A (en) * | 1993-05-21 | 1994-12-02 | Nec Corp | Narrow band excimer laser |
-
1979
- 1979-07-20 JP JP9307879A patent/JPS5617091A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0468738U (en) * | 1990-10-29 | 1992-06-18 | ||
JPH06334253A (en) * | 1993-05-21 | 1994-12-02 | Nec Corp | Narrow band excimer laser |
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