CN104597605A - Beam shaping method for reducing QCL (quantum cascade laser) terahertz source diffraction effect and divergence angle - Google Patents
Beam shaping method for reducing QCL (quantum cascade laser) terahertz source diffraction effect and divergence angle Download PDFInfo
- Publication number
- CN104597605A CN104597605A CN201510039709.7A CN201510039709A CN104597605A CN 104597605 A CN104597605 A CN 104597605A CN 201510039709 A CN201510039709 A CN 201510039709A CN 104597605 A CN104597605 A CN 104597605A
- Authority
- CN
- China
- Prior art keywords
- qcl
- beam shaping
- terahertz
- diffraction effect
- terahertz lens
- 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
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/09—Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
- G02B27/0938—Using specific optical elements
- G02B27/095—Refractive optical elements
- G02B27/0955—Lenses
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/09—Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
- G02B27/0927—Systems for changing the beam intensity distribution, e.g. Gaussian to top-hat
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
The invention relates to a beam shaping method for reducing QCL terahertz source diffraction effect and divergence angle. A beam shaping module used in the method is composed of a plurality of terahertz lenses or a mixture of terahertz lens and off-axis parabolic mirrors. Nearly Gaussian distribution beams of small divergence angle are obtained by adjusting the light path of the beam shaping module. The beam shaping method for reducing QCL terahertz source diffraction effect and divergence angle has the advantages of being capable of synchronically reducing the beam divergence angle to obtain nearly Gaussian beam distribution beams of small divergence angle as well as effectively reducing the QCL terahertz source intense diffraction effect due to output end aperture constraint, thereby greatly prompting a QCL terahertz source application research process.
Description
Technical field
The present invention relates to the beam shaping method of a kind of reducing amount qc laser (quantum cascade laser, referred to as QCL) THz source diffraction effect and the angle of divergence.
Background technology
Terahertz (THz) ripple refers to frequency (corresponding wavelength is from 3 millimeters to 30 microns) from 0.1THz to 10THz, electromagnetic wave between millimeter wave and infrared light, has the features such as security, broadband property, " dactylogram characteristic " and penetrability.THz ripple has important scientific value and wide application prospect, has unique advantage in multiple fields such as basic science, investigation of materials, biomedicine, national public safeties.
THz source generally includes free electron laser, works in the gas laser of Terahertz frequency range, vacuum electronics THz source, ultrafast laser pump light conductance THz source, QCL THz source and photonics THz source and other semiconductor electronic cosmogonys etc.Because QCL THz source not only has higher power level, and there is the advantages such as energy conversion efficiency is high, volume is little, light and easy of integration, therefore thought by academia a terahertz emission source most possibly realizing through engineering approaches and industrialization.
At present, the maximum power output of QCL THz source reaches 250mW, and maximum operating temperature is 186K, and lowest operating frequency is 1.2THz, if externally-applied magnetic field, minimum sharp radio frequency rate can arrive 0.68THz.Along with improving constantly of device performance, QCL THz source is more and more obvious at the potential application advantage in the fields such as imaging, communication and heterodyne detection.
The quality of beam quality be affect device can one of the key factor obtaining practical application.QCL THz source is greater than device size, the especially thickness of device usually due to its resonance wavelength, and the beam cross section EDS maps that it is exported presents strong diffraction effect, disperses full-shape and is usually greater than 60 degree.
Summary of the invention
The strong diffraction effect brought is limited in order to overcome QCL THz source due to output terminal aperture, the present invention adds light beam shaping module in the transmission light path that QCL THz source is follow-up, not only effectively can reduce QCL THz source due to output terminal aperture limits the strong diffraction effect brought, and can beam divergence angle be reduced, obtain the nearly Gaussian distribution light beam of small divergence angle, this brings great impetus by the applied research of QCL THz source.
The technical solution adopted for the present invention to solve the technical problems is: a kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence, described device adopts light beam shaping module, described module is made up of multi-disc Terahertz lens, or to be mixed with off-axis paraboloidal mirror by Terahertz lens and form.By regulating light beam shaping module light path, obtain the nearly Gaussian distribution light beam of small divergence angle.
The invention has the beneficial effects as follows, while effectively reduction QCL THz source limits due to output terminal aperture the strong diffraction effect brought, synchronously can reduce beam divergence angle, obtain the nearly Gaussian distribution light beam of small divergence angle, this will advance the applied research process of QCL THz source greatly.
Accompanying drawing explanation
Describe exemplary embodiment of the present invention in more detail by referring to accompanying drawing, above and other aspect of the present invention and advantage will become and more be readily clear of, in the accompanying drawings:
Fig. 1 is structural representation of the present invention.
A1.QCL THz source in figure, a2. Terahertz lens, a3. Terahertz lens, a4. Terahertz planar array detector, b1. off-axis paraboloidal mirror, b2. off-axis paraboloidal mirror.
Embodiment
Hereinafter, more fully the present invention is described now with reference to accompanying drawing, various embodiment shown in the drawings.But the present invention can implement in many different forms, and should not be interpreted as being confined to embodiment set forth herein.On the contrary, provide these embodiments to make the disclosure will be thoroughly with completely, and scope of the present invention is conveyed to those skilled in the art fully.
Hereinafter, with reference to the accompanying drawings exemplary embodiment of the present invention is described in more detail.
With reference to accompanying drawing 1, in Fig. 1 (a), the output light of QCL THz source a1, after the Terahertz lens combination shaping that a2 and a3 forms, adopts Terahertz planar array detector a4 can monitor the nearly Gaussian distribution hot spot of small divergence angle; In Fig. 1 (b), the off-axis paraboloidal mirror group parallelization that the output light of QCL THz source a1 is made up of b1 and b2 after Terahertz lens a2 focuses on, Terahertz planar array detector a4 can monitor the nearly Gaussian distribution hot spot of small divergence angle; In Fig. 1 (c), the off-axis paraboloidal mirror group that the output light of QCL THz source a1 forms through b1 and b2 is collected and parallelization, again through the Terahertz lens combination shaping of a2 and a3 composition, Terahertz planar array detector a4 can monitor the nearly Gaussian distribution hot spot of small divergence angle; In Fig. 1 (d), the output light of QCL THz source a1 is after the Terahertz lens combination shaping that a2 and a3 forms, again through the off-axis paraboloidal mirror group parallelization of b1 and b2 composition, Terahertz planar array detector a4 can monitor the nearly Gaussian distribution hot spot of small divergence angle.
The foregoing is only embodiments of the invention, be not limited to the present invention.The present invention can have various suitable change and change.All any amendments done within the spirit and principles in the present invention, equivalent replacement, improvement etc., all should be included within protection scope of the present invention.
Claims (6)
1. reduce a beam shaping method for QCL THz source diffraction effect and the angle of divergence, it is characterized in that:
Described method adopts light beam shaping module, and described module is made up of multi-disc Terahertz lens, or mix with off-axis paraboloidal mirror by Terahertz lens and form, by adjustment light beam shaping module light path, and the nearly Gaussian distribution light beam of acquisition small divergence angle.
2. reduce a light-beam forming unit for QCL THz source diffraction effect and the angle of divergence, it is characterized in that:
Described device adopts light beam shaping module, and described module is made up of multi-disc Terahertz lens, or to be mixed with off-axis paraboloidal mirror by Terahertz lens and form.
3. a kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence as claimed in claim 2, is characterized in that:
Described light beam shaping module is the Terahertz lens combination that Terahertz lens (a2) form with Terahertz lens (a3).
4. a kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence as claimed in claim 2, is characterized in that:
The off-axis paraboloidal mirror group that described light beam shaping module is Terahertz lens (a2) and is made up of off-axis paraboloidal mirror (b1) and off-axis paraboloidal mirror (b2) after it.
5. a kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence as claimed in claim 2, is characterized in that:
Described light beam shaping module is the off-axis paraboloidal mirror group that off-axis paraboloidal mirror (b1) and off-axis paraboloidal mirror (b2) form and the Terahertz lens combination be made up of Terahertz lens (a2) and Terahertz lens (a3) after it.
6. a kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence as claimed in claim 2, is characterized in that:
Described light beam shaping module is the Terahertz lens combination be made up of Terahertz lens (a2) and Terahertz lens (a3) and the off-axis paraboloidal mirror group be made up of off-axis paraboloidal mirror (b1) and off-axis paraboloidal mirror (b2) after it.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510039709.7A CN104597605A (en) | 2015-01-27 | 2015-01-27 | Beam shaping method for reducing QCL (quantum cascade laser) terahertz source diffraction effect and divergence angle |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510039709.7A CN104597605A (en) | 2015-01-27 | 2015-01-27 | Beam shaping method for reducing QCL (quantum cascade laser) terahertz source diffraction effect and divergence angle |
Publications (1)
Publication Number | Publication Date |
---|---|
CN104597605A true CN104597605A (en) | 2015-05-06 |
Family
ID=53123500
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201510039709.7A Pending CN104597605A (en) | 2015-01-27 | 2015-01-27 | Beam shaping method for reducing QCL (quantum cascade laser) terahertz source diffraction effect and divergence angle |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN104597605A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109901086A (en) * | 2019-03-29 | 2019-06-18 | 电子科技大学 | A kind of matched quasi-optical cellular construction of realization wave beam |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004085359A (en) * | 2002-08-27 | 2004-03-18 | Tochigi Nikon Corp | Terahertz pulse light measuring device |
CN101663575A (en) * | 2007-08-31 | 2010-03-03 | 佳能株式会社 | Imaging method and apparatus using terahertz radiation |
US7683778B2 (en) * | 2006-02-15 | 2010-03-23 | Canon Kabushiki Kaisha | Apparatus for detecting information on object |
CN102243167A (en) * | 2011-04-01 | 2011-11-16 | 深圳大学 | Terahertz wave imaging device |
CN204462543U (en) * | 2015-01-27 | 2015-07-08 | 中国工程物理研究院激光聚变研究中心 | A kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence |
-
2015
- 2015-01-27 CN CN201510039709.7A patent/CN104597605A/en active Pending
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004085359A (en) * | 2002-08-27 | 2004-03-18 | Tochigi Nikon Corp | Terahertz pulse light measuring device |
US7683778B2 (en) * | 2006-02-15 | 2010-03-23 | Canon Kabushiki Kaisha | Apparatus for detecting information on object |
CN101663575A (en) * | 2007-08-31 | 2010-03-03 | 佳能株式会社 | Imaging method and apparatus using terahertz radiation |
CN102243167A (en) * | 2011-04-01 | 2011-11-16 | 深圳大学 | Terahertz wave imaging device |
CN204462543U (en) * | 2015-01-27 | 2015-07-08 | 中国工程物理研究院激光聚变研究中心 | A kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109901086A (en) * | 2019-03-29 | 2019-06-18 | 电子科技大学 | A kind of matched quasi-optical cellular construction of realization wave beam |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103346056B (en) | The Terahertz slow wave structure of two-stage series connection | |
CN105207042B (en) | A kind of too hereby wave radiation source with oval groove optical grating construction | |
Garufo et al. | A connected array of coherent photoconductive pulsed sources to generate mW average power in the submillimeter wavelength band | |
CN102566198A (en) | Terahertz wave optical parametric amplification device and method thereof | |
CN204462543U (en) | A kind of light-beam forming unit reducing QCL THz source diffraction effect and the angle of divergence | |
CN103779763B (en) | A kind of Terahertz power source high-frequency structure based on array grating structure | |
CN103094025B (en) | A kind of high-power millimeter wave and terahertz emission source apparatus | |
CN104597605A (en) | Beam shaping method for reducing QCL (quantum cascade laser) terahertz source diffraction effect and divergence angle | |
CN204497564U (en) | A kind of laser realizing 2 mu m waveband broad tuning narrow-linewidth lasers and export | |
CN105044841A (en) | Terahertz wave polarization beam splitter based on multiple dielectric cylinder structures | |
Gallerano et al. | High power THz sources and applications at ENEA-Frascati | |
CN105372758A (en) | Bar-type terahertz wave polarization beam splitter | |
Shams et al. | Characterization of terahertz antennas using photoinduced coded‐aperture imaging | |
CN112701554B (en) | Terahertz wave generation method and system based on rydberg atom excitation four-wave mixing | |
Smirnov | Characterization of coherent Cherenkov radiation source | |
Pan et al. | A novel high-gain directional lens antenna for terahertz band | |
Zhang et al. | Generation of broadband THz airy beams applying 3D printing technique | |
CN104682186A (en) | Laser for realizing 2-micron waveband tuning narrow linewidth laser output | |
CN112670799B (en) | Multi-frequency terahertz radiation source based on optimized difference frequency | |
CN204086728U (en) | A kind of Terahertz electric-field enhancing device guided wave structure formed with air-gap conical gradual change | |
CN104155825A (en) | Large-energy terahertz pulse generation method and device | |
CN104570406B (en) | THz wave modulator approach, device and device based on artificial surface plasma | |
CN103368042A (en) | Terahertz source equipment based on semiconductor ultra-short pulsed laser | |
Pillai et al. | Optimization analysis of a nano-dot photoconductive antenna | |
CN112670793B (en) | Multi-frequency terahertz wave generating device based on optimized cascade difference frequency |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
RJ01 | Rejection of invention patent application after publication |
Application publication date: 20150506 |
|
RJ01 | Rejection of invention patent application after publication |