CN100451730C - Beam splitting device and method of linear polarization laser double-pulse of adjustable pulse space - Google Patents
Beam splitting device and method of linear polarization laser double-pulse of adjustable pulse space Download PDFInfo
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- CN100451730C CN100451730C CNB2007100364135A CN200710036413A CN100451730C CN 100451730 C CN100451730 C CN 100451730C CN B2007100364135 A CNB2007100364135 A CN B2007100364135A CN 200710036413 A CN200710036413 A CN 200710036413A CN 100451730 C CN100451730 C CN 100451730C
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Abstract
A light beam splitting device of linearly polarized laser dipulse type with pulse interval being able to be regulated consists of a Faraday light isolator, a passive Fabry-Perot resonantor with electro-optical crystal Pockels cell and a power supply of electro-optical crystal Pockels cell. The said device can device a linearly polarized laser pulse to be a dipulse with its interval and energy ratio both being able to be regulated and controlled. Its beam splitting method is also disclosed.
Description
Technical field
The present invention relates to laser, particularly a kind of beam splitting arrangement and beam-splitting method of linearly polarized laser dipulse of adjustable pulse interval, this device the linearly polarized laser pulse of a finite pulse width (wavelength near ultraviolet near infrared range) can be divided into have optical axis, dipulse that the direction of propagation is identical with the polarization direction, that the recurrent interval can be regulated as required.
Background technology
In laser is used, usually need laser pulse (being designated as " mother lode dashes ") with a linear polarization to be divided into to have optical axis, the direction of propagation is identical with the polarization direction, two subpulses of recurrent interval and beam splitting adjustable ratio.
In general, beam splitting method typically uses that the combination of the beam splitter of suitable transmitance and completely reflecting mirror finishes.The beam splitting ratio of beam splitter is fixed, and different beam splitting ratios will be changed beam splitter; And to obtain same optical axis, the identical direction of propagation and same polarization direction, and recurrent interval and pulse energy be than two subpulses can regulating arbitrarily, and its adjusting work complexity is loaded down with trivial details, the divided beam system poor stability, and whole beam splitting process can cause losing half energy that mother lode dashes.
In the existing technology, Shang Weijian can not lose the beam-splitting method of same optical axis, same propagation direction and the same polarization direction of half energy that mother lode dashes.
Summary of the invention
The objective of the invention is to provide a kind of beam splitting arrangement and beam-splitting method of linearly polarized laser dipulse of adjustable pulse interval, this device can be divided into a linearly polarized laser pulse two, and to have optical axis, the direction of propagation and a polarization direction identical, and recurrent interval, pulse energy are than the subpulse that can regulate as required.That apparatus of the present invention take up room is little, be divided on the principle and do not have the beam energy loss in the subpulse process, has and regulates accurately, simple and convenient, easily advantage such as control.
Technical solution of the present invention is as follows:
A kind of beam splitting arrangement of linearly polarized laser dipulse of adjustable pulse interval, the formation of this device is to be provided with successively on same optical axis: first polarizer, Faraday polarization apparatus, second polarizer, the electro-optic crystal Pockels' cell and first completely reflecting mirror, described first polarizer and second polarizer to see through axle at 45, described first polarizer, the Faraday polarization apparatus and second polarizer constitute a Faraday isolator, in the reflected light direction of described second polarizer is one can be along second completely reflecting mirror of beam direction vertical moving, described first completely reflecting mirror, the electro-optic crystal Pockels' cell, second polarizer and second completely reflecting mirror constitute a passive Fabry-Perot cavity, apply controlled at interval on the two poles of the earth of described electro-optic crystal Pockels' cell respectively, the pulse voltage that amplitude is adjustable.
Apply controlled at interval on the two poles of the earth of described electro-optic crystal Pockels' cell respectively, the circuit of the pulse voltage that amplitude is adjustable constitutes: a synchronous signal connects the input end of synchronizing relay device, this synchronizing relay device is dual output synchronizing relay device different delayed time and that delay time adjustable that has of a single input, the first output termination, first driver of this synchronizing relay device, the second output termination, second driver of this synchronizing relay device, first DC high-voltage power supply connects first electrode of described electro-optic crystal Pockels' cell by described first driver, for described electro-optic crystal Pockels' cell provides the first high direct voltage V
i, second DC high-voltage power supply connects second electrode of described electro-optic crystal Pockels' cell by described second driver, for described electro-optic crystal Pockels' cell provides the second high direct voltage V=V
λ/ 4.
The electro-optic crystal of described electro-optic crystal Pockels' cell is KD
*P, KDP or lithium columbate crystal.
Described faraday's optoisolator be constant magnetic or electromagnetic type drive.
Described first polarizer and second polarizer are thin film polarizer, or the polarizing prism of being made by the birefringece crystal of kalzit, quartz, vanadic acid yttrium.
Utilize above-mentioned beam splitting arrangement, obtain to have the method for optical axis, the direction of propagation and polarization direction dipulse light beam identical, adjustable pulse interval, be characterised in that to comprise the following steps:
1. at t
0In time, is engraved on first electrode of described electro-optic crystal Pockels' cell and applies the first high direct voltage V
i, a linearly polarized laser pulse by the reflection of first completely reflecting mirror, behind twice described electro-optic crystal Pockels' cell of process, is poured out rate T by second polarizer by energy by the input of first polarizer, through the Faraday polarization apparatus and second polarizer
iPour out the 1st lasertron pulse p, the 1st lasertron pulse p sees through second polarizer oppositely by Faraday polarization apparatus, departed from incident direction by first polarizer reflection and propagates the described rate T that pours out
i=cos
2[δ (V
i)/2], in the formula:
For being added with V
iThe pairing retardation of electro-optic crystal Pockels' cell of voltage, V
λAll-wave magnitude of voltage by the corresponding optical maser wavelength of electro-optic crystal Pockels' cell;
2. and then at t
1Constantly, decorporating is added in voltage on the electro-optic crystal Pockels' cell, i.e. V
i=0, carry the dump energy ratio and be (1-T
i) laser pulse s by second polarizer reflection, in described resonator cavity, vibrate;
3. laser pulse s in the chamber, vibrated (n-1) inferior after, and then at t
N-1Constantly, add the second high direct voltage V=V on second electrode of electro-optic crystal Pockels' cell again
λ/ 4, then in the chamber, vibrate t after n time of laser pulse s
nConstantly, pulse is all through second polarizer in the chamber, this pulse sees through second polarizer and oppositely passes through Faraday polarization apparatus, departed from incident direction and propagate second lasertron pulse s by first polarizer reflection, the 2nd lasertron pulse s has the identical pulse in optical axis, the direction of propagation and polarization direction with described the 1st lasertron pulse p.
The time interval between described the 1st lasertron pulse and the 2nd the lasertron pulse is determined by formula:
τ＝2Ln/c，
In the formula: L is that the chamber of laserresonator is long, and n is that laser pulse is at t
N-1-t
1The number of times of vibration in the inherent chamber of time, c is the light velocity.
Technique effect of the present invention is as follows:
By the above as can be known, utilize the beam splitting arrangement of the linearly polarized laser dipulse of adjustable pulse interval of the present invention, a linearly polarized laser pulse can being divided into two, to have optical axis, the direction of propagation and a polarization direction identical, and recurrent interval, pulse energy are than the subpulse that can regulate as required.
That apparatus of the present invention take up room is little, be divided on the principle and do not have the beam energy loss in the subpulse process, the energy that the energy sum of two subpulses of generation is almost dashed near original mother lode.Recurrent interval can be regulated as required by length L of regulating resonator cavity and the frequency n that pulse is vibrated in the chamber.Have and regulate accurately, simple and convenient, advantages such as easy control.
For the laser pulse width for the treatment of beam splitting is the pulse of psec to femtosecond, and the long L in chamber decides at interval with required pulse; And when the laser pulse width for the treatment of beam splitting was tens nanoseconds, separate two pulses, the numerical value of the long L of corresponding cavity is bigger.
Apparatus and method of the present invention, suitable equally for the beam splitting of non-linear polarization ray laser pulse:
(a) for the circularly polarized light laser pulse, with a slice quarter wave plate circularly polarized light is converted to linearly polarized light earlier, carry out beam splitting with device of the present invention again.When being output as circularly polarized light, can with a quarter wave plate output line polarization laser spike train be converted to circularly polarized light again as need.
(b) for the elliptically polarized light laser pulse, the wave plate that postpones with a slice appropriate phase is converted to linearly polarized light with elliptically polarized light earlier, carries out beam splitting with device of the present invention again.Still be the elliptic polarization light time as need output, can with the same wave plate that postpones of a slice output line polarization laser spike train be converted to elliptically polarized light again.
(c) for the nonpolarized light laser pulse, method and apparatus of the present invention is suitable for beam splitting equally, and but, laser pulse can lose part energy by faraday's optoisolator the time, but output still is two linearly polarized laser pulses.
Description of drawings
Fig. 1 is the structural representation of laser pulse beam splitting regulator of the present invention
Fig. 2 is for applying the circuit structure block diagram of pulse voltage on two electrodes of electro-optic crystal Pockels' cell
The pulse voltage waveform figure of Fig. 3 in the electro-optic crystal chamber, being applied on the Pockels' cell
Fig. 4 is the instance graph that utilizes two pulses of apparatus of the present invention generation.
Among the figure:
The pulse of 1-linearly polarized laser
2-first polarizer
The 3-Faraday polarization apparatus
4-second polarizer
5-electro-optic crystal Pockels' cell
6-first completely reflecting mirror
7-second completely reflecting mirror
The direction of 8-output subpulse row
9-faraday optoisolator
The passive Fabry-Perot cavity of 10-
The 11-second completely reflecting mirror translation direction
The 21-synchronizing signal
22-synchronizing relay device
23-first driver
24-first DC high-voltage power supply
25-resistance
26-electric capacity
27-second DC high-voltage power supply
28-second driver
31-is added in the first high direct voltage pulse voltage waveform on first electrode of electro-optic crystal Pockels' cell
32-is added in the second high direct voltage pulse voltage waveform on second electrode of electro-optic crystal Pockels' cell
In fact 33-is added in the assembled pulse voltage waveform on the electro-optic crystal Pockels' cell
Embodiment
The invention will be further described below in conjunction with embodiment and accompanying drawing, but should not limit protection scope of the present invention with this.
See also Fig. 1 and Fig. 2 earlier, Fig. 1 is the structural representation of beam splitting arrangement of the linearly polarized laser dipulse of adjustable pulse interval of the present invention, apply the circuit structure block diagram of pulse voltage on two electrodes of Fig. 2 for the electro-optic crystal Pockels' cell in passive Fabry-Perot cavity, as seen from the figure, the formation of the beam splitting arrangement of the linearly polarized laser dipulse of adjustable pulse interval of the present invention is to be provided with successively on same optical axis: first polarizer 2, Faraday polarization apparatus 3, second polarizer 4, the electro-optic crystal Pockels' cell 5 and first completely reflecting mirror 6, described first polarizer 2 and second polarizer 4 to see through axle at 45, described first polarizer 2, the Faraday polarization apparatus 3 and second polarizer 4 constitute a Faraday isolator, in the reflected light direction of described second polarizer 4 is one can be along second completely reflecting mirror 7 of beam direction vertical moving, described first completely reflecting mirror 6, electro-optic crystal Pockels' cell 5, second polarizer 4 and second completely reflecting mirror 7 constitute a passive Fabry-Perot cavity 10.
The circuit that applies pulse voltage on the two poles of the earth of described electro-optic crystal Pockels' cell 5 constitutes: a synchronous signal 21 connects the input end of synchronizing relay device 22, this synchronizing relay device 22 be a single input have different delayed time and synchronizing relay device that delay time adjustable dual output, the first output termination, first driver 23 of this synchronizing relay device 22, the second output termination, second driver 28 of this synchronizing relay device 22, first DC high-voltage power supply 24 connects first electrode of described electro-optic crystal Pockels' cell 5 by described first driver 23, for described electro-optic crystal Pockels' cell 5 provides the first high direct voltage V
i, second DC high-voltage power supply 27 connects second electrode of described electro-optic crystal Pockels' cell 5 by described second driver 28, for described electro-optic crystal Pockels' cell 5 provides the second high direct voltage V=V
λ/ 4.
The signal that described synchronizing relay device 22 is added in first driver 23 and second driver 28 has sequencing, t as shown in Figure 3
1And t
N-1Constantly.t
1, t
N-1With respect to t
0Can regulate continuously.Utilize synchronizing relay device 22 to regulate continuously, to be first DC high-voltage power supply 24 connect first electrode of described electro-optic crystal Pockels' cell 5 by described first driver 23 to voltage waveform 31, for described electro-optic crystal Pockels' cell 5 provides the first high direct voltage V
iVoltage waveform, to be second DC high-voltage power supply 27 connect second electrode of described electro-optic crystal Pockels' cell 5 by described second driver 28 to voltage waveform 32, for described electro-optic crystal Pockels' cell 5 provides the second high direct voltage V=V
λ/ 4 voltage waveform.In fact the driving voltage waveform that obtains of electro-optic crystal Pockels' cell 5 two ends is the above two difference, and promptly voltage waveform 33, t
0It is the initial moment that synchronizing signal 21 is applied to the voltage waveform 31 on first electrode of described electro-optic crystal Pockels' cell 5.
The electro-optic crystal of described electro-optic crystal Pockels' cell 5 is KD
*P, KDP or lithium columbate crystal.
Described faraday's optoisolator 9 be constant magnetic or electromagnetic type drive.
Described polarizer is a thin film polarizer, or the polarizing prism of being made by the birefringece crystal of kalzit, quartz, vanadic acid yttrium.
Utilize described beam splitting arrangement, the process of method that obtains to have optical axis, the direction of propagation and polarization direction dipulse light beam identical, adjustable pulse interval is as follows:
Because described faraday's optoisolator 9 is a kind of unidirectional opticses that pass through: forward (as among Fig. 1 from left to right) linearly polarized laser of incident can be losslessly by faraday's optoisolator. but oppositely the light of (among the figure from right to left) incident can not be by faraday's optoisolator from former input path outgoing, and departs from former incident direction and along 8 outgoing.
The passive Fabry-Perot cavity that contains electro-optic crystal Pockels' cell 5 is made of second polarizer 4, electro-optic crystal Pockels' cell 5, first completely reflecting mirror 6 and second completely reflecting mirror 7.First completely reflecting mirror, 6, the second completely reflecting mirrors 7 are vertical with incident ray respectively, so constitute a resonator cavity.When not applying voltage on the electro-optic crystal Pockels' cell 5, the laser pulse that someways falls in the chamber into can vibration back and forth in resonator cavity 10, can not export.
If it is W that the linearly polarized laser mother lode dashes 1 gross energy, be divided into two same optical axises, the same propagation direction, and recurrent interval, pulse energy than the subpulse that can regulate as required, the concrete operations step is as follows:
I) t
0In time, is engraved in electro-optic crystal Pockels' cell 5 and adds a voltage V
iMake the laser mother lode consistent with the direction of the axis of homology of first polarizer 2 towards 1 polarization direction, behind first polarizer 2 and Faraday polarization apparatus 3, laser polarization direction is rotated 45 degree, and consistent with the axis of homology of second polarizer 4, losslessly by second polarizer 4.The laser mother lode dashes 1 by being added with V
iAfter the electro-optic crystal Pockels' cell 5 of voltage came and went twice, polarization state changed, and becomes elliptically polarized light, and the mother lode of this elliptic polarization is punched in and is decomposed into two mutually perpendicular polarized components on second polarizer 4: s polarized component and p polarized component.Wherein the p polarized component is propagated along direction shown in 8 by first polarizer reflection oppositely by second polarizer 4 and Faraday polarization apparatus 3, has exported the 1st subpulse p thus, and its energy is WT
i
At this, the energy in definition chamber is poured out rate T
iBe the energy Wp of p polarized component in the elliptically polarized light in the chamber and the ratio of elliptically polarized light gross energy We, this numerical value is by the making alive V of institute on the electro-optic crystal Pockels' cell 5
iDetermine:
T
i＝cos
2[δ(V
i)/2] (a)
The retardation of the correspondence that this electro-optic crystal Pockels' cell 5 is produced is:
Ii) mother lode dashes 1 by being added with V
iThe t that the electro-optic crystal Pockels' cell 5 of voltage comes and goes after twice
1Constantly, decorporating is added in voltage on the electro-optic crystal Pockels' cell 5, i.e. V
i=0.Carry dump energy W (1-T
i) the pulse of s polarized component reflected into resonator cavity 10 by second polarizer 4 and vibrate.
Iii) the pulse of s polarized component in the chamber, vibrated (n-1) inferior after, and then at t
N-1Constantly, give making alive V on the Pockels' cell 5
λ/ 4, V wherein
λFor 5 pairs of electro-optic crystal Pockels' cells should optical maser wavelength the all-wave magnitude of voltage, t
N-1=t
1+ 2L (n-1)/c, wherein L is the effective optical length between first completely reflecting mirror 6 and second completely reflecting mirror 7, c is the light velocity.Then carry of the pulse of dump energy ratio, the t in the chamber after vibration n time for the s polarized component of (1-Ti)
nConstantly, all through second polarizer 4.Obtained second lasertron pulse s thus.The exit direction of this pulse s is identical with the exit direction of first subpulse p.
The time interval of two pulses is τ=2Ln/c, (completely reflecting mirror 7 can move along the axis in chamber the long L in chamber that can be by regulating resonator cavity, 11 usefulness double-head arrows are represented in the drawings) and the pulse frequency n of in the chamber, vibrating controlled, can adjust by synchronizing relay device 22 on apparatus of the present invention, the energy ratio of two pulses is by getting V
iNumerical value determine, promptly regulate by the output of first DC high-voltage power supply 24.
Adopt apparatus and method of the present invention, with a 1064nm laser pulse, be input into the device of forming by faraday's optoisolator 9, Pockels' cell 5 and first completely reflecting mirror 6 and second completely reflecting mirror 7 by mode shown in Figure 1 by the 15ns of Nd:YAG laser instrument generation.Get cavity length L and be about 4.8 meters, the used time τ of pulse round trip in the chamber is about 32ns.A pulse is divided into energy equates that the recurrent interval is respectively the dipulse of 32ns.The result of output gap 32ns dipulse as shown in Figure 4.
Claims (7)
1, a kind of beam splitting arrangement of linearly polarized laser dipulse of adjustable pulse interval, the formation that is characterised in that this device is to be provided with successively on same optical axis: first polarizer (2), Faraday polarization apparatus (3), second polarizer (4), electro-optic crystal Pockels' cell (5) and first completely reflecting mirror (6), described first polarizer (2) is at 45 through axle with second polarizer (4), described first polarizer (2), Faraday polarization apparatus (3) and second polarizer (4) constitute a Faraday isolator (9), in the reflected light direction of described second polarizer (4) is one can be along second completely reflecting mirror (7) of beam direction vertical moving, described first completely reflecting mirror (6), electro-optic crystal Pockels' cell (5), second polarizer (4) and second completely reflecting mirror (7) constitute a passive Fabry-Perot cavity (10), apply controlled at interval on the two poles of the earth of described electro-optic crystal Pockels' cell (5) respectively, the pulse voltage that amplitude is adjustable.
2, the beam splitting arrangement of the linearly polarized laser dipulse of adjustable pulse interval according to claim 1, it is characterized in that applying respectively on the two poles of the earth of described electro-optic crystal Pockels' cell (5) controlled at interval, the circuit of the pulse voltage that amplitude is adjustable constitutes: a synchronous signal (21) connects the input end of synchronizing relay device (22), this synchronizing relay device (22) is dual output synchronizing relay device different delayed time and that delay time adjustable that has of a single input, first output termination first driver (23) of this synchronizing relay device (22), second output termination second driver (28) of this synchronizing relay device (22), first DC high-voltage power supply (24) connects first electrode of described electro-optic crystal Pockels' cell (5) by described first driver (23), for described electro-optic crystal Pockels' cell (5) provides the first high direct voltage V
i, second DC high-voltage power supply (27) connects second electrode of described electro-optic crystal Pockels' cell (5) by described second driver (28), for described electro-optic crystal Pockels' cell (5) provides the second high direct voltage V=V
λ/ 4, V
λAll-wave magnitude of voltage for the corresponding optical maser wavelength of electro-optic crystal Pockels' cell.
3, the beam splitting arrangement of the linearly polarized laser dipulse of adjustable pulse interval according to claim 1 is characterized in that the electro-optic crystal of described electro-optic crystal Pockels' cell (5) is KD
*P, KDP or lithium columbate crystal.
4, the beam splitting arrangement of the linearly polarized laser dipulse of adjustable pulse interval according to claim 1, it is characterized in that described Faraday isolator (9) be constant magnetic or electromagnetic type drive.
5, the beam splitting arrangement of the linearly polarized laser dipulse of adjustable pulse interval according to claim 1, it is characterized in that described first polarizer (2) and second polarizer (4) they are thin film polarizer, or by kalzit or by polarizing prism quartzy or that make by the birefringece crystal of vanadic acid yttrium.
6, utilize the described beam splitting arrangement of claim 1 to obtain to have the method for optical axis, the direction of propagation and polarization direction dipulse light beam identical, adjustable pulse interval, be characterised in that to comprise the following steps:
1. at t
0In time, is engraved on first electrode of described electro-optic crystal Pockels' cell (5) and applies a voltage V
iA linearly polarized laser pulse (1) is by first polarizer (2) input, through Faraday polarization apparatus (3) and second polarizer (4), by first completely reflecting mirror (6) reflection, behind twice described electro-optic crystal Pockels' cell of process (5), poured out rate T by energy by second polarizer (4)
iPour out the 1st lasertron pulse p, the 1st lasertron pulse p sees through second polarizer (4) oppositely by Faraday polarization apparatus (3), departed from incident direction and propagates the described rate T that pours out by first polarizer (2) reflection
i=cos
2[δ (V
i)/2], in the formula: V
iFor being added in first high direct voltage on the electro-optic crystal Pockels' cell (5);
For being added with V
iThe pairing retardation of electro-optic crystal Pockels' cell (5) of voltage, V
λAll-wave magnitude of voltage for the corresponding optical maser wavelength of electro-optic crystal Pockels' cell;
2. and then at t
1Constantly, decorporating is added in voltage on the electro-optic crystal Pockels' cell (5), i.e. V
i=0, carry the dump energy ratio and be (1-T
i) laser pulse s by second polarizer (4) reflection, in described resonator cavity, vibrate;
3. laser pulse s in the chamber, vibrated (n-1) inferior after, and then at t
N-1Constantly, add the second high direct voltage V=V on second electrode of electro-optic crystal Pockels' cell (5) again
λ/ 4, then in the chamber, vibrate t after n time of laser pulse s
nConstantly, pulse is all through second polarizer (4) in the chamber, this pulse sees through second polarizer (4) oppositely by Faraday polarization apparatus (3), departed from incident direction and propagate second lasertron pulse s by first polarizer (2) reflection, this second lasertron pulse s has the identical pulse in optical axis, the direction of propagation and polarization direction with described the 1st lasertron pulse p.
7, acquisition according to claim 6 has the method for optical axis, the direction of propagation and polarization direction dipulse light beam identical, adjustable pulse interval, it is characterized in that the time interval between described the 1st lasertron pulse and second the lasertron pulse is determined by formula:
τ＝2Ln/c，
In the formula: L is that the chamber of laserresonator is long, and n is that laser pulse is at t
N-1-t
1The number of times of vibration in the inherent chamber of time, c is the light velocity.
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|---|---|---|---|
| CNB2007100364135A CN100451730C (en) | 2007-01-12 | 2007-01-12 | Beam splitting device and method of linear polarization laser double-pulse of adjustable pulse space |
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|---|---|---|---|
| CNB2007100364135A CN100451730C (en) | 2007-01-12 | 2007-01-12 | Beam splitting device and method of linear polarization laser double-pulse of adjustable pulse space |
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| CN102856372B (en) * | 2012-09-28 | 2015-12-09 | 中国科学院苏州纳米技术与纳米仿生研究所 | The encapsulating structure of double grid four end group III-nitride enhancement mode HEMT device |
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| CN104238123B (en) * | 2014-07-15 | 2016-08-24 | 天津理工大学 | The common light path ultrashort laser pulse beam-splitting method at adjustable pulse interval and beam splitting arrangement |
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