上海玻色智能科技有限公司是一家仪器设备的代理与系统集成业务的综合性服务商，总部设在上海，业务覆盖国内各高校、*所属各研究所、*所属各研究所、航空工业总公司所属各研究所等不同系统内的研究机构，以及相关领域内的各大生产型公司。

玻色由具有丰富的仪器设备应用和使用经验的人员组成，我们不仅仅代理设备，我们同时提供基于各种设备本身的各种拓展应用和研发。公司代理的主要产品有海洋光学的光纤光谱仪等，我们在光纤光谱仪行业有着多年的工作经验，积累了大量的应用和研发实例，可以为客户提供一站式的解决方案。

点击展示更多内容

产品简介在线询价

ISOMET声光调制器,声光偏转器,声光移频器,AOTF,声光可调谐滤波器ISOMET公司主要生产各种声光器件，包括声光调制器,声光偏转器,声光移频器,AOTF,声光可调谐滤波器

ISOMET声光调制器产品详情

ISOMET声光调制器, 声光偏转器, 声光移频器, AOTF, 声光可调谐滤波器

ISOMET公司主要生产各种声光器件，包括声光调制器, 声光偏转器, 声光移频器, AOTF, 声光可调谐滤波器。

声光调制器件由声光介质和压电换能器构成。当驱动源的某种特定载波频率驱动换能器时,换能器即产生同一频率的超声波并传入声光介质,在介质内形成折射率变化，光束通过介质时即发生相互作用而改变光的传播方向即产生衍射。声光调制是一种外调制技术，通常把控制激光束强度变化的声光器件称作声光调制器。声光调制技术比光源的直接调制技术有高得多的调制频率；与电光调制技术相比，它有更高的消光比（一般大于1000：1），更低的驱动功率，更优良的温度稳定性和更好的光点质量以及低的价格；与机械调制方式相比，它有更小的体积、重量和更好的输出波形。

All AO devices feature a piezo-electric transducer bonded to one face of a crystal material. When an RF drive signal is applied to this transducer, a travelling acoustic wave is generated in the crystal. Due to the photo-elastic effect the acoustic column produces a periodic change in the refractive index, similar in effect to the slits of a diffraction grating. Practical AO devices are designed such that a high proportion of the incident laser light is diffracted into a single output order. This is operation in the Bragg regime.

ISOMET声光调制器, 声光偏转器, 声光移频器, AOTF, 声光可调谐滤波器

Bragg diffraction requires a defined interaction length (L), and the laser light to be input at a specific angle. The Bragg and separation angles are a function of the optical wavelength, the RF drive frequency and the crystal acoustic velocity (V). Some AO crystal types require the input beam to be polarized.
The RF drive frequency determines the output angle of the diffracted beam and the RF power determines the beam intensity. These are the basic control mechanisms of AO modulators and deflectors.

声光调制器 Acousto-optics Modulators

Acousto-optic modulators (AOM) are used to control laser beam intensity.

This can be simple ON:OFF modulation for fast switching or variable level modulation to provide proportional intensity control. These modes are determined by the RF driver type; digital or analog modulation respectively (or a combination of both).

The RF drive frequency is typically fixed and the RF amplitude is modulated accordingly.

The optical rise and fall time is defined by the laser beam diameter in the AOM and the crystal acoustic velocity. For high modulation rates, the beam will need to be focused at the AOM.

Model	Crystal Material	Active App(mm)	Typical Risetime (ns)	Typical Modulation Freq. (MHz)	Center Freq. (MHz)	Suggested Driver Fixed or Variable Frequency	Feature
Single Beam Modulators: UV - Blue
M1062-FS40L-5.5	Fused Silica	5.5	600	0.6	40	Fixed / Variable
M1211-aQ110-5U	Quartz	5	570	0.6	110	Fixed / Variable	Low WF Distortion
M1211-aQ150-3U	Quartz	2.7	230	1.5	150	Fixed / Variable	Low WF Distortion
M1212-aQ150-2	Quartz	2	113	6	150	Fixed / Variable	UV
M1134-FS80L	Fused Silica	3	109	3	80	Fixed / Variable
M1136B-FS80L-H	Fused Silica	2001/2/3	108	10	80	Fixed / Variable
M1088-FS110L	Fused Silica	3	109	3	110	Fixed / Variable	UV
M1133U-aQ110L	Quartz	1	57	6	110	Fixed / Variable	UV
M1211-aQ150-2U	Quartz	2	57	6	150	Fixed / Variable	UV
1206C-2-1002	TeO2	2	30	12	110	Fixed / Variable	NUV, VIS
M1211-aQ150-2U	Quartz	2	25	14	150	Fixed / Variable	UV
M1212-aQ175	Quartz	1	20	18	175	Fixed / Variable	UV
1206C-833	TeO2	1	15	25	110	Fixed / Variable	NUV, VIS
M1212-aQ200	Quartz	0.8	10	30	175	Fixed / Variable	UV
1250C-829A	TeO2	0.45	9	40	260	Fixed / Variable	NUV, VIS

Single Beam Modulators: Blue - Red
OAM1020	TeO2 (S)	3	2000	0.2	110	Fixed / Variable
OAM1060	TeO2 (S)	2	1000	0.3	80	Fixed / Variable
M1115-FS80L-3	Fused Silica	3(H)x14(W)	170	2	80	Fixed / Variable
M1133-aQ80L	Quartz	1.5 / 2	114	3	80	Fixed / Variable
M1201E-SF40-1.7	Glass	1.7	46	8	40	Fixed / Variable
1205C-x	PbMo04	2001/2/3	25	15	80	Fixed / Variable
M1211-aQ110-3	Quartz	2.7	57	6	110	Fixed / Variable	Low WF Distortion
1206C	PbMo04	1	15	25	110	Fixed / Variable
1206C-833	TeO2	1	15	25	110	Fixed / Variable
1206C-2-1002	TeO2	2	30	12	110	Fixed / Variable
1250C	PbMo04	0.75	10	40	200	Fixed / Variable
1250C-829A	TeO2	0.45	9	40	260	Fixed / Variable
1250C-848	TeO2	0.5	7	50	200	Fixed / Variable
1250C-974	TeO2	0.4	7	50	200	Fixed / Variable
M1067-T200L	TeO2	0.2	7	50	200	Fixed / Variable
1260C	TeO2	0.2	6	100	350	Fixed / Variable

Single Beam Modulators: NIR
M1312-T80L	TeO2	6	700	0.5	80	Fixed / Variable	Hi Pwr
1202-4	Glass	4 x 14(W)	350	1	40	Fixed / Variable
1203-3	Fused Silica	3 x 14(W)	350	1	60	Fixed / Variable
M1099-T80L	TeO2	3	300	1.2	80	Fixed / Variable
M1135-T80L	TeO2	3	300	1.2	80	Fixed / Variable	Hi Pwr
M1137-SF40L	Glass	1.5	191	2	40	Fixed / Variable
M1133-aQ80L	Quartz	1	114	3	80	Fixed / Variable
M1201E-SF40-1.7	Glass	1.7	90	4	40	Fixed / Variable
M1080-T80L	TeO2	1.5	80	4	80	Fixed / Variable
1205C-1023	PbMo04	0.6	50	7	80	Fixed / Variable
M1142-SF80L	Glass	0.5	40	10	80	Fixed / Variable
1205C-x-NIR	PbMo04	0.5	30	12	80	Fixed / Variable
1205C-843	PbMo04	0.5	25	15	80	Fixed / Variable
1206C-NIR	PbMo04	1	20	18	110	Fixed / Variable
1250C-868	TeO2	0.5	15	23	150	Fixed / Variable
1250C-NIR	PbMo04	0.75	12	30	200	Fixed / Variable

Single Beam Modulators: Mid IR - IR
1210-G(fc)-H-MIR	Ge	2,4	240	10	60- 105	Fixed / Variable
M1208-G80-4-MIR	Ge	4x8	500	10	80	Fixed / Variable	New version of 1208-6-4-MIR
M1189-G40-4	Ge	4	470	0.7	40	Fixed / Variable
M1208-G40-3	Ge	3x8	350	1	40	Fixed / Variable	New version of 1208-4-955M
1209-7-1064M	Ge	7x14	830	0.4	40	Fixed / Variable
1209-7-1112M	Ge	7x14	830	0.4	40	Fixed / Variable
1209-9-1010M	Ge	9x20	940	0.4	40	Fixed / Variable
AOM650-H	Ge	7,8,9x30	830	0.4	50	Fixed / Variable
AOM640-H	Ge	7,8,9x30	830	0.4	40	Fixed / Variable
AOM740-H	Ge	7,8,9x30	830	0.4	40	Fixed / Variable
M1199-G40-H	Ge	7,8,9x30	700	0.5	40	Fixed / Variable	Pulsed lasers
M1310-G40-H	Ge	7,8,9x30	700	0.5	40	Fixed / Variable	Pulsed lasers
M1315-G40	Ge	6,7,8,9x15	700	0.5	40	Fixed / Variable
M1192-G40-12	Ge	12 x 30	1200	0.3	40	Fixed / Variable	Large aperture

Dual Beam Modulators
AOM650-9	Ge	9 x 30	600	0.6	40 / 60
M1199-G50-9	Ge	9 x 30	600	0.6	40 / 60		Pulsed lasers
DBM1172-G41-9	Ge	9 x 20	600	0.6	43 / -43
DBM1186-G54-9	Ge	9 x 20	600	0.6	54 / -54
DBM1199-G54-9	Ge	9 x 20	600	0.6	54 / -54

Multichannel Modulators
Model	Channels	Material	Active Aperture (mm)	Typical Risetime (ns)	Information Bandwidth (MHz)	Center Freq. (MHz)	Feature
M1140	4	PbMoO4	0.7	25	15	110
G7060	6	Ge	0.8	70	5	70
M8080	8	PbMoO4	0.5	55	6	80
M9080C	8	PbMoO4	0.7	36	9	90	colinear o/p
M15080	8	Quartz	0.7	70	5	110

Modulators with Integrated Driver
Model	Std A/R	Optical Material	Max Aperture (mm)	Typical Risetime (ns)	Typical Modulation Freq. (MHz)	Center Freq. (MHz)	Mod
IMAD-P80L	VIS	PbMo04	1.5	25	15	80	Analog
IMDD-P80L	VIS	PbMo04	1.5	25	15	80	Digital
IMAD-T110L	405nm	TeO2	1.5	25	15	110	Analog
IMDD-T110L	405nm	TeO2	1.5	25	15	110	Digital
IMAA-P80L	VIS	PbMo04	1.5	25	15	80	Amp Only

声光移频器 Frequency Shifters

All AO devices apply a frequency shift to the diffracted output beams. Acousto-optic frequency shifters (AOFS) are compact devices designed specifically for this task. Depending on the selected Bragg angle, these devices will either up-shift or down-shift the laser light by the frequency of the applied RF signal. Two or more devices can be cascaded in order to achieve sum or difference frequency combinations. Compound absorber angles are incorporated to minimize acoustic reflections.

Model	Std A/R	Crystal Material	Active App (mm)	Centre Freq(MHz)	Tuning BW (MHz)	Suggested Driver Fixed or Variable Frequency	Feature
OAM1059-V31	633nm	TeO2 (S)	1.5	+/-10	+/- 0.5	Fixed / Variable	+ and - shift
OAM1059A	633nm	TeO2 (S)	1.5	15	+/- 1.0	Fixed / Variable
FS1303-TxxxR-J2	NIR	TeO2 (S)	2	xxx	+/- 1.0	Fixed / Variable
OAM1141-TxxS-2	633nm	TeO2 (S)	2	40 / 80	+/- 1.0	Fixed / Variable
M1136A-FS40S-1	UV	FS (S)	1	40	+/- 5	Fixed / Variable
1205C-1-869	633nm	PbMo04	0.7	80	+/- 15	Fixed / Variable
1205-1054	VIS	PbMo04	1	80	+/- 5	Fixed / Variable
M1141-P80-1	VIS	PbMo04	1	80	+/- 5	Fixed / Variable
1205-1118	VIS,NIR	PbMo04	2	80	+/- 5	Fixed / Variable
M1136B-FS80L-H	UV	FS (L)	1/2/3	80	+/- 5	Fixed / Variable
1206C	VIS,NIR	PbMo04	1	110	+/- 25	Fixed / Variable
1205-1069	VIS	PbMo04	1	160	+/- 5	Fixed / Variable
1250C	VIS,NIR	PbMo04	0.75	200	+/- 50	Fixed / Variable
1250C-829A	NUV,VIS	TeO2	0.45	260	+/- 50	Fixed / Variable
OPP-1	VIS	PbMoO4	1.5	300	+/- 100	Fixed / Variable
1260C	NUV,VIS	TeO2	0.2	350	+/- 100	Fixed / Variable
1209-7-1064M	IR	Ge	6	40	+/- 10	Fixed / Variable
1210-G-(fc)-H-MIR	Mid-IR	Ge	2,4	60 / 105	+/- 10	Fixed / Variable
M1208-G80-3	IR	Ge	3	80	+/- 2.5	Fixed / Variable

声光偏转器 Deflectors

AO deflectors can be used to scan a laser beam. This is achieved by changing the RF drive frequency. Random position, continuous line scans and sequential spot deflection are all possible. Scan rates in excess of 250KHz can be achieved depending on the crystal, wavelength and beam size.

Optimum efficiency requires that the input laser beam is set at the Bragg angle which is a function of the drive frequency. When swept to scan the laser beam there will be Bragg angle mismatch since the AOD can only be optically aligned at one drive frequency. In general this will cause a reduction in efficiency depending on the scan range. Several techniques may be used to minimize this effect:

Off-axis AO deflectors (“OAD”) minimize the Bragg angle - frequency sensitivity by exploiting non-linear characteristics of birefringent crystals.
Beam steered AO deflectors (“-BS”) electronically steer the acoustic column inside the crystal depending on the RF drive frequency. This requires a phased array electrode on the transducer with 2 or 4 RF inputs.

Model	A/R Coating	Material	Rayleigh Res'n 1 2	Aperture (mm)	Sweep BW (MHz)	Center Freq. (MHz)	Feature
Deflectors UV - Blue
D1211-aQ110-5	UV	Quartz	70	5 x 10	40	110
D1340-XY-aQ110-5	UV	Quartz	35 x 35	5 x 5	40	110	Dual Axis
D1155-T75S	405nm	TeO2 (S)	140	9	10	75
1206C-2-1002	NUV, VIS	TeO2	100	2 x 9	50	110

Deflectors Blue - Red
1205C-2-804B	VIS	PbMoO4	66	2 x 6	30	80
LS55-V	VIS	TeO2 (S)	450	2 x 7	40	80
LS110A-VIS	VIS	TeO2 (S)	1100	4 x 14	50	100
LS110A-VIS-XY	VIS	TeO2 (S)	750x750	9 x 9	50	100	Dual Axis
OAD948	488nm	TeO2 (S)	600	3 x 8	50	100
OAD1020	532nm	TeO2 (S)	600	2 x 8	50	100
1206C-2-1002	NUV, VIS	TeO2	77	2 x 8	50	110
OPP834	VIS	PbMoO4	520	0.7 x 19	100	200
1250C-BS-960A	VIS	PbMoO4	160	1.5 x 6	120	190
D1135-T180L	VIS	TeO2	95	3 x 8	50	175

Deflectors - Near IR
OAD1550-XY	1550nm	TeO2 (S)	200 x 200	7 x 7	20	40
LS110A-NIR	NIR	TeO2 (S)	550	4 x 14	25	50
LS110A-NIR-XY	NIR	TeO2 (S)	240 x 240	6 x 6	25	50
1205C-x-804B	NIR	PbMoO4	66	2 x 6	40	80
OAD1121-XY	810nm	TeO2 (S)	500 x 500	9 x 9	40	80
LS55-NIR	NIR	TeO2 (S)	450	2 x 7	40	80
D1312-T80L	NIR	TeO2	40	6	30	80
D1086-T110L	NIR	TeO2	95	3 x 8	50	110	Conduction cooled
D1135-T110L	NIR	TeO2	95	3 x 8	50	110
1250-BS-926	NIR	PbMoO4	60	0.5 x 3	70	145
1250C-BS-943A	NIR	PbMoO4	190	2 x 6	120	185

Deflectors Mid IR - IR
1209-7BS-986	IR	Ge	50	7 x 14	20	40
D1315-G50-H	IR	Ge	70	7 x 20	20	50
AOM650-H	IR	Ge	100	7 x 30	20	50
D1199-G50	IR	Ge	100	7 x 20	20	50
D1208-XY-50-3	IR	Ge	10 x 10	3 x 3	40	70
LS700-1011	IR	Ge	436	10 x 60	40	70

可调滤光片Tunable Filters

Acousto-optic diffraction requires momentum matching between light and sound (acoustic) waves in the crystal material. For the AO laser beam modulator, momentum matching is maximized when the input beam is aligned at the Bragg angle. AOTF applications are different. Unlike the modulator case, AOTF’s are frequently used with non-coherent, poorly collimated light and require large apertures with wide acceptance angles. To accommodate these demands, AOTF’s utilize non-linear properties of birefringent crystals. The crystal orientation and acoustic launch angle are designed such that diffraction occurs over a very narrow wavelength range for a very specific RF frequency. In fact it is so specific that multiple simultaneous frequencies can be applied to an AOTF without excessive intermodulation. This allows controlled wavelength mixing.
The acoustic launch angle and incident angle are related by design and together define the AOTF characteristics.

Model	Spectral Range (um)	Active Aperture (sq. mm)	Acceptance Angle (Deg.)	Optical BW (nm)	Drive Frequency (MHz)
Visible Tunable Filters
AOLF615-1049	VIS	2.5x2.5	3.5 - 4.5	1.0 - 6.0	109 - 65
AOLF615-1082	VIS	2.5x2.5	3.5 - 4.5	1.0 - 6.0	109 - 65
AOTF614-08	VIS,NIR	5x5	3.5 - 6.0	1.0 - 22.0	140 - 35
AOTF614-16	VIS,NIR	5x5	2.5 - 4.2	0.6 - 11.0	140 - 35
AOTF614-24	VIS,NIR	5x5	3.5 - 6.0	0.4 - 7.0	140 - 35
AOTF1331	mid-IR	7x7	5	30 - 50	24 - 39
AOTF1110-VB	VIS,NIR	10x10	5.7 (nominal)	Variable	80 - 50

NIR - IR Tunable Filters
AOTF614-08	VIS,NIR	5x5	3.5 - 6.0	1.0 - 22.0	140 - 35
AOTF614-16	VIS,NIR	5x5	2.5 - 4.2	0.6 - 11.0	140 - 35
AOTF614-24	VIS,NIR	5x5	3.5 - 6.0	0.4 - 7.0	140 - 35
AOTF920-14	NIR	5x5	3.4 - 6.1	2.0 - 27.0	95 - 26
AOTF920-20	NIR	5x5	2.6 - 4.9	1.5 - 18.5	95 - 26
AOTF920-24	NIR	5x5	2.8 - 5.0	1.0 - 15.5	95 - 26
AOTF1331	mid-IR	7x7	5	30 - 50	24 - 39
AOTF1550-SLS	1550nm	3x3	-	2	81 - 84
AOTF1110-VB	VIS,NIR	10x10	5.7 (nominal)	Variable	80 - 50

Q-Switches

Q-switches are intracavity devices used to generate very high peak power, short duration laser pulses. These are typically loss modulators operating on the zero order beam. The goal of a Q-switch is to diffract as much power from the zero order as possible to increase the cavity loss and extinguish the laser output. When the RF drive to the Q-switch is momentarily turned off, the optical power built up in the laser is emitted as a short pulse. The process may be repeated at rates in excess of 100KHz. Depending on the frequency and interaction length, AO Q-switches either operate in the Bragg regime, just like an AOM, with predominately a single diffracted beam or in the Raman-Nath regime with multiple diffracted beams.

Model	Cooling	Centre Frequency (MHz)	Material	Active Aperture (mm)	Max Power (W)	Damage Thresh (MW/cm^2)	Driver
Q1072-SF24L	Conduction	24	SF10	1.5	5	>300	AQS
Q1058C-SFxxL-H	Conduction	24/27	SF10	1.0/1.5	5	>300	AQS
Q1025-TxxL-H	Conduction	27/80	TeO2	1	3	>250	AQS
Q1025-SFxxL-H	Conduction	41/80	SF10	1	3	>300	AQS
Q1080C-TxxL-H	Conduction	41/ 68 / 80	TeO2	1.5	4	>250	AQS
Q1087-aQ80L	Conduction	80	Quartz	1	6	>500	AQS
Q1137-SFxxL-H	Conduction	41/80	SF57	1.0 / 1.5	6	>300	AQS
Q1162-SFxxL-H	Conduction	41/80	SF10	1	6	>300	AQS
Q1119-aQxxL-H	Conduction	41/ 80	Quartz	1.0 / 1.5	10	>500	AQS
Q1119-FSxxL-H	Conduction	41/ 80	Fused Silica	1.0 / 1.5	10	>500	AQS
Q1133-aQxxL-H	Conduction	41/ 68 / 80	Quartz	1.0 to 2.0	10	>500	AQS
Q1133-FSxxL-H	Conduction	41/ 68 / 80	Fused Silica	1.0 / 1.5	10	>500	AQS
Q1062-FSxxL-H	Water	24/ 27	Fused Silica	1.5 to 6.0	60	>500	AQS
Q1062-FSxxS-H	Water	24/ 27	F.Silica (Shear)	1.5 to 5.5	60	>500	AQS
Q1083-FSxxL-H	Water	24/ 27 / 41	Fused Silica	1.5 to 6.0	60	>500	AQS
Q1083-FSxxS-H	Water	24/ 27 / 41	F.Silica (Shear)	1.5 to 5.5	60	>500	AQS

Special Function Devices

Model	Operating Wavelengths	Material	Resolution	Time Aperture (us)	Sweep Bandwidth (MHz)	Center Freq. (MHz)
OPP-1	VIS	PbMoO4	1000	5	200	300
OPT-1	VIS	TeO2 (S)	1500	50	30	45
OPT-1-100	VIS	TeO2 (S)	5000	100	50	75
SLM16-835	NIR	TeO2	300	4.4	70	125
LS700-1109-10W	IR	Ge	500	10	50	75

Fiber Optic Couplers

For ease of integration ISOMET offers a range of pre-aligned fibre assemblies and integrated fibre coupled devices for both modulation and frequency shifting applications. The FOA series offers an open and fully adjustable fibre coupling solution suitable for use with a wide range of our visible and NIR AO devices. The FCM series are fully integrated welded package fibre coupled devices. These exhibit high extinction ratio, low coupling losses and feature single mode fibres with FC/PC terminations.

Model	Applications	Wavelengths	Suitable AOM’s	Typical Coupling Losses
FOA1065	Frequency Shifting / Modulation	Visible and NIR	1205C / 1206C / 1250C	< 5dB
FOA1084	High Speed Modulation	NIR	1206C – 0.5	< 5dB
FCM1550-P50L	Frequency Shifting / Modulation	1550nm	Integrated	< 3dB
FCM1550-P80L	Frequency Shifting / Modulation	1550nm	Integrated	< 3dB

声光调制器驱动器 Acousto-optics Modulators Driver

Center Freq (MHz)	Risetime (n sec)	Digital Modulation		Analog Modulation		Power	Feature
10	<15			831C		up to 0.3W
27	<10	521C-27	521B-27	531C-27	531B-27	up to 6W
40	<8	521C	521B	531C	531B	up to 6W
45	<8	521C-45	521B-45	531C-45	531B-45	up to 6W
80	<6	522C	522B	532C	532B	up to 7W
80	<6	822C		832C		up to 2W	Low voltage, compact
110	<5	523C	523B	533C	533B	up to 6W
150	<5	524C	524B	534C	534B	up to 3W
175	<5	525C-175	525B-175	535C-175	535B-175	up to 2W
200	<5	525C	525B	535C	535B	up to 2W
250 (260)	<5	526C		536C		up to 2W
350	<5			537C		up to 1.5W
80	<6	752C-x	752B-x	752C-x	752B-x	up to 7W	Dual Modulation
80	<6	722C-x	722B-x	na	na	up to 6W	>60dB RF Contrast
110	<5	723C-x	723Bx	na	na	up to 6W	>60dB RF Contrast

Air Cooled, Single Frequency up to 60W RF power
Frequency (Select, MHz)	Model	Frequency Stability (Typical, %)	Modulation	Outputs	RF Power (W)
24/27/41/80/110	RFA910-FC	±0.003	Analog& Digital	1	10
24/27/41/80/110	RFA920-FC	±0.003	Analog & Digital	1	25
27/41	RFA960-FC	±0.003	Analog & Digital	1	60

High Power Modulator Drivers Liquid Cooled
Frequency (MHz)	Model	Modulation	Outputs	RF Power (W)	Feature
40	RFA141	Analog & Digital	1	30
40	RFA241	Analog & Digital	1	80
40	RFA441	Analog & Digital	1	100
40	RFA641	Analog & Digital	1	180	Digital Interface
50	RFA151	Analog & Digital	1	25
60	RFA261	Analog & Digital	1	65
80	RFA181	Analog & Digital	1	50
110	RFA2110	Analog & Digital	1	25
40	RFA240-2	Analog & Digital	2	70/70
50	RFA250-2	Analog & Digital	2	70/70

Liquid Cooled, Sequential Multi-Frequency, up to 180W RF power
Frequency (MHz)	Model	Frequency Stability (Typical, %)	Modulation	Outputs	RF Power (W)	Feature
30 / 50	RFA3050-2	± 0.003	Digital	2	65/65
40 / 51	RFA741	± 0.003	Analog/Digital	1	90
40 / 60	RFA4060-2	± 0.003	Digital	2	65/65
40 / 60	RFA4116-2	± 0.003	Digital	2	85/85	Digital Power Control
30 / 36.7 / 43.3 / 50	RFA3445-2	± 0.003	Digital	2	85/85
40 / 46.7 / 53.3 / 60	RFA4556-2	± 0.003	Digital	2	85/85
30-60	iSPA241	32Bit	Analog / Digital	1	70	USB Programmable
35-55	iSPA641	32Bit	Analog / Digital	1	180	USB Programmable
40-60	iSPA4060-2	32Bit	Analog / Digital	2	85/85	USB Programmable
41/-41	iSA241-4	32Bit	Analog / Digital	4	30/30/30/30	DBM driver
54/-54	iSA254-4	32Bit	Analog / Digital	4	45/45/45/45	DBM driver

声光偏转器驱动器 Deflectors Drivers

Variable Frequency Driver-Amps Conduction Cooled Max 20W
Tuning Frequency (Minimum, MHz)	Digital Modulation	Analog Modulation	Tuning Linearity (Typical, %)	RF Power (W)	Feature
DDS Based
20-200	iSPA-SF1	iSPA-SF1	32Bit	1.2W	Sequential freq output
20-200	iSPA-MF4	iSPA-MF4	32Bit	<1W	Simultaneous 4x freq output
Single Output VCO based
19-35	620C-27	630C-27	±2.0	>2.2
30-50	620C-40	630C-40	±1.5	>2.2
30-50	620A-40	630A-40	±1.5	>6.0
60-100	620C-80	630C-80	±1.5	>2.2
60-100	620A-80	630A-80	±1.5	>4.0
70-130	620C-100	630C-100	±1.5	>2.0
80-140	620C-110	630C-110	±1.5	>1.8
80-140	620A-110	630A-110	±1.5	>3.0
100-200	620C-150	630C-150	±1.5	>1.5
100-200	620A-150	630A-150	±1.5	>3.0
140-260	620C-200	630C-200	±1.5	>1.5
200-300	620C-250	630C-250	±2	>0.7
250-450	620C-350	630C-350	±2	>0.7
22-38		RFA910T-30	±2.5	10
30-50		RFA910T-40	±1.5	10
60-100		RFA910T-80	±1.5	10
60-100		RFA920T-80	±1.5	20
90-130		RFA920T-110	±1.5	20
VXCO
80 ± 4kHz		512C-x		Up to 7

Multi Output Variable Freq Driver-Amps Conduction Cooled, Max 20W
Tuning Frequency (Minimum, MHz)	Digital Modulation	Analog Modulation	Tuning Linearity (Typical, %)	RF Power (W)	Outputs	Feature
DDS Based
20-200	iSPA-SF2		32Bit	1.2/1.2	2	USB Programmable
20-200	iHSA-4*		32Bit	1.2/1.2/1.2/1.2	4	USB Programmable
VCO Based
30-50 or 40-60	D321-BS	D331-BS	±1	1.8 / 1.8	2
50-90	D322-BS	D332-BS	±1	1.8 / 1.8	2
75-125 or 90-130	D323-BS	D333-BS	±1	1.8 / 1.8	2
120-240 or 130-250	D325-BS	D335-BS	±1	1.8 / 1.8	2
85-145	RFA3110-4-CC		±1.5	1.8/1.8/1.8/1.8	4

Liquid Cooled, up to 180W RF power
Tuning Frequency (Minimum, MHz)	Model	Tuning Linearity (Typical, %)	Modulation	Outputs	RF Power (W)	Feature
DDS Based
30-60	iSPA241	32Bit	Analog / Digital	1	70	USB Programmable
30-60	iSPA241	32Bit	Analog / Digital	1	70	USB Programmable
40-60	iSPA4060-2	32Bit	Analog / Digital	4	85/85	USB Programmable
VCO Based
30-50	RFA321	±2	Analog / Digital	1	70
30-50	RFA331-2	±2	Analog / Digital	2	35/35
40-60	RFA350-2	±2	Analog / Digital	2	65/65
65-95	RFA3080-2	±1.5	Analog / Digital	2	5/5
90-130	RFA333-2	±1.5	Analog / Digital	2	10/10
85-145	RFA3110-4	±1.5	Analog / Digital	4	1.8/1.8/1.8/1.8
110-180	RFA 3145-4	±1.5	Analog / Digital	4	1.8/1.8/1.8/1.8
130-210	RFA3175-4	±1.5	Analog / Digital	4	1.5/1.5/1.5/1.5

AOTF Driver: Frequency Sources and Amps

Frequency Sources
Model	Controls Functions	Max tuning range (MHz)	Resolution	Outputs	RF Power	Feature
Frequency Synthesizer Source
iSA-SF2	Yes	20-200	32bit	2	1mW	USB programmable
iHHS-4	Yes	20-200	32bit	4	1mW	USB programmable
iHHS-4-e	Yes	150-350	32bit	4	1mW	USB programmable
Synthesizer with Integrated Amplifier(s)
iSPA-SF1-X	Yes	20-250	32bit	1	1W to 4W	High power
iSPA-SF2	Yes	20-200	32bit	2	1W	Differential frequency
iSPA-MF4	Yes	20-200	32bit	1	1W total	Mixed frequency
iHSA-4	Yes	20-200	32bit	4	1W	Image Memory
Crystal Based, low frequency
811C-L-10		10	50ppm	1	300mW
811C-L-15		15	50ppm	1	300mW

Amplifiers
Model	Modulation Input	Octave Bandwidth within range (MHz)	Gain (dB)	Outputs	RF Power (W)	Feature
50xC-L Series	Yes	30-250	0-33	1	1.7
50xC-2 Series	Yes	30-250	0-34	1	2
50xC-3 Series	Yes	30-250	0-35	1	2.7
50xC-6 Series	Yes	30-250	0-36	1	6.5
DA134-p-fc	Yes	30-150	0-36	2	1.6/1.6
RFA901-B	Yes	30-100	0-38	1	12
RFA200	Yes	28-55	0-50	1	70
RFA200-2	Yes	28-55	0-50	2	70/70
RFA1170-4-ZP	No	48-92	52	4	80/80/80/80	Pulse optimized
RFA1170-4	Option	48-92	52	4	80/80/80/80

Q-Switch Drivers
Frequency (MHz)	Model	Waveform Modulation	Control Inputs	Outputs	RF Power
24	RFA960-24	Analog & Digital	User	1	60
27.12	RFA960-27	Analog & Digital	User	1	60
27.12	AQS1060-27	Pulse Width and Slope Envelope	Internal/User	1	60
27.12	AQS1080-27	Pulse Width and Slope Envelope	Internal/User	1	80
27.12	AQSR1100D-27	Pulse Width and Slope Envelope	Internal/User	2	110/110
40.68	RFA910-40	Analog & Digital	User	1	12
40.48	RFA960-40	Analog & Digital	User	1	60
40.68	AQS1010-40	Pulse Width and Slope Envelope	Internal/User	1	10
80	762B-x	Preset Pulse Width		1	< 4
80	762C-x	Preset Pulse Width		1	< 4
80	RFA910-80	Analog & Digital	User	1	12
80	AQS1004-80	Pulse Width and Slope Envelope	Internal/User	1	< 6
80	AQS1010-80	Pulse Width and Slope Envelope	Internal/User	1	12

热门产品

产品名称	参考价	地区	公司名称	更新时间
烟气含湿量检测器	￥8000	青岛市	青岛路博建业环保科技有限公司	2024-04-19	在线询价
自动测量图像尺寸设备	￥560000	深圳市	深圳市中图仪器股份有限公司	2024-03-04	在线询价
罗卓尼克USB接口水活性快速测量探头	面议	无锡市	无锡徽科特测控技术有限公司	2024-05-13	在线询价
高通量实时荧光检测分析系统	面议	上海市	美谷分子仪器（上海）有限公司	2024-02-28	在线询价
激光功率测量系统 LPMS	面议		上海倍蓝光电科技有限公司	2024-04-23	在线询价
水分活度测量仪厂商	面议	常州市	常州金坛泰纳仪器厂	2023-08-24	在线询价

免责申明

所展示的信息由会员自行提供，内容的真实性、准确性和合法性由发布会员负责，仪表网对此不承担任何责任。仪表网不涉及用户间因交易而产生的法律关系及法律纠纷，纠纷由您自行协商解决

友情提醒：本网站仅作为用户寻找交易对象，就货物和服务的交易进行协商，以及获取各类与贸易相关的服务信息的平台。为避免产生购买风险，建议您在购买相关产品前务必确认供应商资质及产品质量。过低的价格、夸张的描述、私人银行账户等都有可能是虚假信息，请采购商谨慎对待，谨防欺诈，对于任何付款行为请您慎重抉择！如您遇到欺诈等不诚信行为，请您立即与仪表网联系，如查证属实，仪表网会对该企业商铺做注销处理，但仪表网不对您因此造成的损失承担责任！