JP2009194418A - Atomic oscillator - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide an atomic oscillator having high precision and low power consumption by improving a Q value by reducing optical intensity to reduce the full width at half maximum of an EIT signal, and by improving a S/N ratio. <P>SOLUTION: This atomic oscillator includes an LD 53 to emit each kind of resonance light, a resonance gas cell 58 to pass each kind of resonance light in a metal atom gas, a PD 55 to detect transmitting light 1, a beat component detecting means 2 to detect a difference frequency beat component in a received photoelectric current, a detecting means 3 to detect the amplitude level of the difference frequency beat component detected by the beat component detecting means 2, a frequency control means 59 to generate the control voltage of a crystal oscillator 60 based on the detected output of the detecting means 3, the crystal oscillator 60 to oscillate a predetermined frequency based on the control voltage generated from the frequency control means 59, and a modulating means 61 to modulate the dc current of the LD (coherent light source) 53 by a modulation frequency ω<SB>m</SB>generated by synthesizing and multiplying the oscillating frequency of the crystal oscillator 60. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

  The present invention relates to an atomic oscillator, and more particularly to a circuit technique for increasing the detection accuracy of an EIT signal in a CPT type atomic oscillator.

  An atomic oscillator using an alkali metal such as rubidium or cesium needs to keep atoms in a gas state when utilizing energy transition of atoms, and therefore operates a gas cell in which atoms are hermetically sealed while maintaining a high temperature. . The principle of operation of an atomic oscillator is broadly divided into a double resonance method using light and microwaves, and a method using a quantum interference effect (hereinafter referred to as CPT: Coherent Population Trapping) by two types of laser light. In both cases, the amount of the light incident on the gas cell is detected by the detector provided on the opposite side to detect how much light has been absorbed by the atomic gas, so that the atomic resonance is detected and a reference signal from a crystal oscillator or the like is sent to the control system. Output is obtained in synchronization with atomic resonance.

FIG. 6A is a schematic diagram illustrating a modulation method of a coherent light source. This modulation method is called a direct modulation method, and a DC power source 51 (direct current) is modulated by a modulation frequency ω _m 52 and supplied to a laser diode (LD) 53 to emit light. As a result, when the EIT phenomenon occurs as shown in FIG. 6B, the frequency component of the light 54 produced by directly modulating the LD 53 is 1 / of the frequency that resonates with the carrier frequency ω _o and the energy level. The coupling optical frequency ω _c and the probe optical frequency ω _p detuned by 2 from the carrier frequency ω _o are obtained. These lights that passed through the resonance gas cell 58 detected a direct current component as a light receiving current of the photodiode (PD) 55 (see FIG. 7). FIG. 8 is a diagram showing a schematic configuration of a conventional atomic oscillator. Conventionally, as described above, a DC component is detected as the light receiving current of the PD 55, and the current value is converted into a voltage by the I / V converter 57 and input to the frequency control means 59. However, since the amount of change in the DC component is very weak, measures have conventionally been taken to increase the S / N ratio of the signal.
As a prior art of an atomic oscillator in the CPT system, Patent Document 1 discloses an atomic oscillator that uses a small gas cell to improve accuracy.
JP 2004-96410 A

However, in the light intensity detection of the conventional optical system disclosed in Patent Document 1, when the gas cell is reduced, the light intensity of the coherent light source is reduced in order to reduce the full width at half maximum of the EIT spectrum and increase the Q value. There was a need. However, if the light intensity is decreased, the level of the EIT signal is also relatively decreased, which causes a problem that the S / N ratio is deteriorated.
The present invention has been made in view of the above problems, and has a circuit configuration capable of detecting a difference frequency beat component included in a signal detected by a photodetector, thereby reducing the light intensity and reducing the half value of the EIT spectrum. An object is to provide an atomic oscillator with high accuracy and low power consumption by increasing the Q value by reducing the overall width and increasing the S / N ratio.

  SUMMARY An advantage of some aspects of the invention is to solve at least a part of the problems described above, and the invention can be implemented as the following forms or application examples.

[Application Example 1]
An atomic oscillator that controls an oscillation frequency by utilizing a light absorption characteristic by a quantum interference effect when two types of resonant light as coherent light having different wavelengths are incident, and a coherent light source that emits each of the resonant lights; A gas cell which is disposed on the emission side of the coherent light source and encloses gaseous metal atoms, allows the resonance light to pass through the metal atom gas, and a light detection means for detecting light passing through the gas cell; and Beat component detection means for detecting a difference frequency beat component included in the light receiving current detected by the light detection means, and detection means for detecting the amplitude level of the difference frequency beat component detected by the beat component detection means. It is characterized by that.

  The atomic oscillator of the present invention utilizes the quantum interference effect of coherent light such as laser light. In this method, two ground levels are simultaneously irradiated in a three-level system (for example, a Λ-type three-level system) in which two ground levels receive resonant light and are resonantly coupled with a common excitation level. Is exactly equal to the energy difference between the ground level 1 and the ground level 2, the three-level system becomes a superposition state of the two ground levels, and the excitation to the excitation level 3 stops. CPT uses this principle to detect and use a state in which light absorption in the gas cell stops when the wavelength of one or both of the two resonance lights is changed. The atomic oscillator of the present invention detects the difference frequency beat component included in the current detected by the light detection means, and obtains the EIT signal by detecting the amplitude level of the difference frequency beat component. As a result, the light intensity can be reduced, the full width at half maximum of the EIT spectrum can be reduced to increase the Q value, and the S / N ratio can be increased to increase the accuracy of the oscillation frequency and reduce the power consumption.

[Application Example 2]
The beat component detection means includes an I / V converter and an amplifier that can operate in a frequency band for modulating the coherent light source.

  As the light detecting means, a photodiode whose light receiving current value varies depending on the light intensity is generally used. In order to detect the modulated microwave frequency component in the light receiving current, it is required to operate with microwaves. In view of this, the present invention is constituted by an I / V converter and an amplifier that detect a current of a microwave frequency component and convert it into a voltage. Thereby, the difference frequency beat component detected by the light detection means can be detected with a simple circuit configuration.

[Application Example 3]
The coherent light source is characterized in that the emission power of the coherent light source is reduced as much as possible in order to reduce the full width at half maximum of the EIT spectrum.

  The present invention detects the difference frequency beat component detected by the light detection means as the EIT signal. Since the difference frequency beat component changes greatly with respect to the change amount of the conventional DC component, the S / N ratio increases. Thereby, the full width at half maximum of the EIT spectrum can be reduced to increase the Q value, and the oscillation frequency can be highly accurate and the power consumption can be reduced.

[Application Example 4]
The modulation method for modulating the coherent light source is a direct modulation method for directly modulating a current supplied to the coherent light source.

The direct modulation method is a method in which a direct current supplied for causing a laser diode to emit light is directly modulated by a modulation frequency (ω _m ). Accordingly, the spectrum components of the emitted laser beam include the carrier light (ω _o ) and the spectrum of the coupling light (ω _c ) and the probe light (ω _p ) detuned from the carrier frequency ω _o by the modulation frequency ω _m. Is done. In the present invention, the difference frequency beat components of ω _o and ω _c and ω _o and ω _p are detected by the photodiode. If the optical electric field amplitude Eo of the carrier light, the optical electric field amplitude Ec of the coupling light, and the optical electric field amplitude Ep of the probe light, the DC component of the received current at this time is proportional to Ec ² + Ep ² , and the difference frequency beat component is It is proportional to EoEc + EoEp. Thereby, when Eo of carrier light is larger than Ec and Ep, the difference frequency beat component becomes larger.

[Application Example 5]
The coherent light is laser light.

  Ordinary light is light in which various wavelengths are mixed and the phase is random. On the other hand, laser light has good monochromaticity in wavelength and is light with a uniform phase. Coherence is defined as a measure of the stability of the wavelength and phase of light. Light with good coherence, that is, with stable wavelength and phase, can cause a quantum interference effect. In that respect, laser light is optimal.

[Application Example 6]
The gaseous metal atom is rubidium or cesium.

  If cesium atoms are used, a highly accurate atomic oscillator can be realized. In addition, rubidium atoms are easy to use because the microwave transition frequency is lower than 6.8 GHz and 9.2 GHz of cesium atoms. Therefore, any metal atom can be selected in consideration of the required performance and convenience of the atomic oscillator.

Hereinafter, the present invention will be described in detail with reference to embodiments shown in the drawings. However, the components, types, combinations, shapes, relative arrangements, and the like described in this embodiment are merely illustrative examples and not intended to limit the scope of the present invention only unless otherwise specified. .
FIG. 1 is a configuration diagram of a main part of an atomic oscillator according to an embodiment of the present invention. The same components will be described with the same reference numerals as in FIG. This atomic oscillator 100 is an atomic oscillator 100 that controls the oscillation frequency by utilizing the light absorption characteristics due to the quantum interference effect when two types of resonant light as coherent light having different wavelengths are incident. An emitted LD (coherent light source) 53, a resonance gas cell 58 that is disposed on the emission side of the LD 53 and encloses gaseous metal atoms and allows each resonance light to pass through the metal atom gas, and light that has passed through the resonance gas cell 58 PD (light detection means) 55 for detecting 1, beat component detection means 2 for detecting a difference frequency beat component included in the current detected by the PD 55, and difference frequency beat component detected by the beat component detection means 2 Detection means 3 for detecting the amplitude level, frequency control means 59 for generating a control voltage of the crystal oscillator 60 based on the detection voltage of the detection means 3, A crystal oscillator 60 for oscillating a frequency defined based on a control voltage generated from the wave number control unit 59, the modulation frequency omega _m produced by synthesis and multiplication based on the oscillation frequency of the crystal oscillator 60 LD (coherent light source) And modulation means 61 for modulating 53 drive currents. Since the gist of the present invention is the optical detection method of the atomic oscillator, a detailed description of the frequency control of the atomic oscillator is omitted.

  That is, the atomic oscillator 100 of this embodiment uses quantum interference of coherent light such as laser light. In this system, in a system in which two ground levels receive resonance light and are resonantly coupled with a common excitation level, the frequencies of the two resonance lights irradiated simultaneously are precisely the ground level 1 and the ground level. When the energy difference of level 2 coincides, the atom is in a superposition state of two ground levels, and excitation to excitation level 3 stops. CPT uses this principle to detect and use a state in which light absorption in the gas cell stops when the wavelength of one or both of the two resonance lights is changed. Further details will be described with reference to FIG. FIG. 2 is an example for explaining a three-level system of atoms by the CPT method. The rubidium and cesium ground levels used in the atomic oscillator are divided into two kinds of ground levels by the hyperfine structure due to the interaction between the nuclear spin I and the total angular momentum J of the electrons. These ground level atoms absorb light and excite to higher energy levels. A state in which two ground levels receive light and are resonantly coupled to a common excitation level as shown in FIG. 2 is called two-photon resonance. In FIG. 2, since the ground level 1 (23) and the ground level 2 (24) have slightly different levels of energy, the resonant light also has a wavelength slightly different from that of the resonant light 1 (20) and the resonant light 2 (22), respectively. Different. When the frequency difference (wavelength difference) between the resonant light 1 (20) and the resonant light 2 (22) irradiated at the same time exactly matches the energy difference between the ground level 1 (23) and the ground level 2 (24), The system shown in FIG. 2 enters a superposition state of two ground levels, and excitation to the excitation level 21 stops. The CPT utilizes this principle to absorb light in the gas cell 3 (that is, to the excitation level 21) when the wavelength of one or both of the resonant light 1 (20) and the resonant light 2 (22) is changed. This is a method of detecting and using a state where the conversion is stopped. The transmitted light that passes through the gas cell 6 in a state where the light absorption is stopped is called an EIT signal.

That is, ordinary light is light in which various wavelengths are mixed and the phase is random. On the other hand, laser light has good monochromaticity in wavelength and is light with a uniform phase. Coherence is defined as a measure of the stability of the wavelength and phase of light. Light with good coherence, that is, with stable wavelength and phase, can cause a quantum interference effect. In that respect, laser light is optimal.
The atomic oscillator 100 of the present invention detects the difference frequency beat component included in the current detected by the PD 55 by the beat component detection means 2 and detects the amplitude level of the difference frequency beat component by the detection means 3. To obtain an EIT signal. As a result, the light intensity can be reduced, the full width at half maximum of the EIT spectrum can be reduced to increase the Q value, and the S / N ratio can be increased to achieve high accuracy and low power consumption.

  FIG. 3 is a diagram showing an example of the circuit configuration of the beat component detecting means of the present invention. The beat component detecting means 2 is constituted by an I / V converter 4 and an amplifier 5 that can operate within a frequency band for modulating the LD 53. That is, as the light detection means, a photodiode whose light receiving current value varies depending on the light intensity is generally used. In order to detect the modulated microwave frequency component in the light receiving current, it is required to operate with microwaves. Therefore, in the present embodiment, the I / V converter 4 and the amplifier 5 are configured to detect the current of the microwave frequency component and convert it into a voltage. Thereby, the difference frequency beat component detected by the PD 55 can be detected with a simple circuit configuration.

FIG. 4 is a diagram for explaining the light detection method of the atomic oscillator of the present invention. For comparison, the characteristics of the conventional DC component are shown in FIGS. 4 (a) and 4 (b). The direct modulation method is a method of directly modulating the DC power source 51 (direct current) for causing the laser diode 53 to emit light with the modulation frequency (ω _m ) as described with reference to FIG. Accordingly, as shown in FIG. 6 (b), as the spectral component of the emitted laser light, the coupling light (ω _c ) detuned from the carrier frequency ω _o by the modulation frequency ω _m together with the carrier light (ω _o ). A spectrum of the probe light (ω _p ) is generated. In the present invention, the difference frequency beat components of ω _o and ω _c and ω _o and ω _p are detected. At this time, assuming that the optical electric field amplitude Eo of the carrier light, the optical electric field amplitude Ec of the coupling light, and the optical electric field amplitude Ep of the probe light, the direct current component of the light receiving current detected by the photodiode 55 is as shown in FIG. in proportional to Ec ² + Ep ^2, difference frequency beat component as shown in FIG. 4 (c), it is proportional to EoEc + EoEp. Thus, when the light intensity emitted from the laser diode 53 is small and the coupling light Ec and the probe light Ep are smaller than the carrier light Eo, the received light current value (Ec ² + Ep ² ) when the DC component resonates. Although the level difference between the light reception current value (FIG. 4 (b)) when not resonating (FIG. 4 (a)) and the difference frequency beat component is small, the light reception current value (EoEc + EoEp) (FIG. 4 (c) )) And the level difference between the received light current values (FIG. 4D) when there is no resonance. That is, the S / N can be increased by detecting the difference frequency beat component generated by the PD 55 as the EIT signal. The difference frequency beat component greatly changes with respect to the amount of change of the conventional DC component, so the S / N ratio increases, so that the light intensity can be reduced. Therefore, the full width at half maximum of the EIT signal can be reduced by reducing the light intensity. It is possible to increase the Q value by reducing the size. As a result, the full width at half maximum of the EIT signal can be reduced to increase the Q value, and the S / N can be improved to increase the accuracy of the oscillation frequency and reduce the power consumption.

FIG. 5 is a diagram illustrating a state of current actually output from the PD. The vertical axis represents PD current and the horizontal axis represents time. As is apparent from this figure, when modulated by the modulation means 56 at the modulation frequency omega _m, component of the modulation frequency omega _m is the difference frequency beat component 11 of the top of the PD current omega _o and omega _c and omega _o and omega _p Appears. The difference frequency beat component 11 is a component in which the frequency band of the amplifier 57 is not detected narrowly because only the DC component is detected in the conventional circuit configuration (FIG. 8). Accordingly, only the DC component 10 appears from the amplifier 57. Therefore, in the present invention, the difference frequency beat component 11 can be detected by the I / V converter 4 and the amplifier 5 having the frequency band of the microwave band as shown in FIG. The beat component detecting means 2 can detect only the difference frequency beat component 11 and detect the EIT signal by detecting the amplitude level by the detecting means 3.

It is a principal part block diagram of the atomic oscillator which concerns on embodiment of this invention. It is a figure explaining the 3 level system of an atom by a CPT system. It is a figure which shows an example of the circuit structure of the beat component detection means of this invention. It is a figure explaining the optical detection method of the atomic oscillator of this invention. It is a figure showing the mode of the light reception current detected by PD. It is a schematic diagram explaining the modulation system of a coherent light source. It is a schematic diagram which shows the structure of the conventional optical system. It is a figure which shows the structure of the conventional atomic oscillator.

Explanation of symbols

  1 transmitted light, 2 beat component detection means, 3 detection means, 4 I / V converter, 5 amplifier, 53 LD, 55 PD, 56, 57 amplifier, 58 resonance gas cell, 59 frequency control means, 60 crystal oscillator, 61 modulation Means, 100 atomic oscillator

Claims (6)

An atomic oscillator that controls an oscillation frequency by utilizing a light absorption characteristic by a quantum interference effect when two types of resonance light as coherent light having different wavelengths are incident,
A coherent light source that emits each resonance light, a gas cell that is disposed on the emission side of the coherent light source, encloses gaseous metal atoms, and passes the resonance light in the metal atom gas, and passes through the gas cell Light detecting means for detecting the detected light, beat component detecting means for detecting the difference frequency beat component included in the current detected by the light detecting means, and amplitude of the difference frequency beat component detected by the beat component detecting means An atomic oscillator comprising: a detecting means for detecting a level.   2. The atomic oscillator according to claim 1, wherein the beat component detecting means includes an I / V converter and an amplifier operable within a frequency band for modulating the coherent light source.   The atomic oscillator according to claim 1 or 2, wherein the coherent light source has a light emission power of the coherent light source made as small as possible in order to reduce the full width at half maximum of the EIT spectrum.   4. The atomic oscillator according to claim 1, wherein the modulation method for modulating the coherent light source is a direct modulation method for directly modulating a current supplied to the coherent light source.   The atomic oscillator according to claim 1, wherein the coherent light is laser light.   The atomic oscillator according to any one of claims 1 to 5, wherein the gaseous metal atom is rubidium or cesium.

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