CN209803572U - Novel optical machine device of two-dimensional magneto-optical trap - Google Patents

Novel optical machine device of two-dimensional magneto-optical trap Download PDF

Info

Publication number
CN209803572U
CN209803572U CN201920425605.3U CN201920425605U CN209803572U CN 209803572 U CN209803572 U CN 209803572U CN 201920425605 U CN201920425605 U CN 201920425605U CN 209803572 U CN209803572 U CN 209803572U
Authority
CN
China
Prior art keywords
reflection mirror
optical trap
dimensional magneto
degree high
wave plate
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.)
Expired - Fee Related
Application number
CN201920425605.3U
Other languages
Chinese (zh)
Inventor
张辉
王心亮
施俊如
白杨
张首刚
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
University of Chinese Academy of Sciences
National Time Service Center of CAS
Original Assignee
University of Chinese Academy of Sciences
National Time Service Center of CAS
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by University of Chinese Academy of Sciences, National Time Service Center of CAS filed Critical University of Chinese Academy of Sciences
Priority to CN201920425605.3U priority Critical patent/CN209803572U/en
Application granted granted Critical
Publication of CN209803572U publication Critical patent/CN209803572U/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Optical Couplings Of Light Guides (AREA)

Abstract

A two-dimensional magneto-optical trap optical-mechanical device is characterized in that a two-dimensional magneto-optical trap cavity is arranged in the middle of an installation platform, an integrated collimating mirror A is arranged on the right front side of the two-dimensional magneto-optical trap cavity, light spots emitted by the integrated collimating mirror A8 penetrate through rectangular windows on the front side and the rear side of the two-dimensional magneto-optical trap cavity and irradiate on a first 45-degree high-reflection mirror group A on the rear side of the two-dimensional magneto-optical trap cavity, and a quarter wave plate A and a zero-degree high-reflection mirror A are sequentially arranged in the reflected light emitting direction of the 45-degree high-reflection mirror group A on the; an integrated collimating mirror B is arranged at the lower right of the two-dimensional magneto-optical trap cavity, light spots emitted by the integrated collimating mirror B penetrate through rectangular windows at the upper side and the lower side of the two-dimensional magneto-optical trap cavity and irradiate on a first 45-degree high-reflection mirror group B arranged above the two-dimensional magneto-optical trap cavity, and a quarter wave plate B and a zero-degree high-reflection mirror B are sequentially arranged in the emergent direction of reflected light of the first 45-degree high-reflection mirror group B arranged below the two-dimensional magneto-optical trap cavity.

Description

Novel optical machine device of two-dimensional magneto-optical trap
Technical Field
The utility model belongs to the technical field of the atomic clock, concretely relates to novel ray apparatus of two dimension magneto-optical trap.
Background
At present, a cold atomic group sample of an atomic clock is pre-cooled generally by adopting a two-dimensional magneto-optical trap, namely, a slow atomic beam is generated firstly, and then the cold atomic sample is cooled and imprisoned by adopting a three-dimensional magneto-optical trap technology to generate the cold atomic sample used for the work of the atomic fountain clock. Because the present atom fountain clock is in pulse type work, atom transition signals are collected discontinuously, in a pulse time gap, the frequency of a reference signal source of the atom clock is not controlled, the noise of the reference source can be reflected on the frequency scale output, and therefore the stability performance of the atom fountain clock is influenced, the time for preparing cold atom samples, namely the shorter the loading time is, the more the stability performance is improved, and the two-dimensional magneto-optical trap precools the atom samples to generate slow atom beams, so that the time for cooling and trapping the atom samples by the three-dimensional magneto-optical trap can be improved, namely the loading time can be shortened.
The current optical-mechanical structure of the two-dimensional magneto-optical trap generally adopts an integrated collimating mirror, a two-dimensional magneto-optical trap cavity (containing gradient magnetic field distribution), a polarization beam splitter prism and a quarter wave plate, as shown in fig. 1. The cooling laser enters the integrated collimating lens barrel through the optical fiber, and then the power of the light beam is uniformly split through a half wave plate and a polarization beam splitter prism in the lens barrel. Two bundles of light pass through corresponding quarter wave plate respectively, form circular polarization light, then rethread two-dimentional magneto-optical trap cavity (contain gradient magnetic field distribution), pass through quarter wave plate again, return incident light through the high mirror of zero degree again to form the laser standing wave field with atom steam interact, when passing atom steam, laser and atom steam interact, slow down the cooling to atom steam in two perpendicular directions, thereby form slow-speed atom and restraint, enter into three-dimensional magneto-optical trap through two-dimentional magneto-optical trap cavity export.
The existing two-dimensional magneto-optical trap device comprises a polarization beam splitter prism, a quarter-wave plate and other polarization devices which are easily influenced by temperature, particularly the number of the quarter-wave plates is large, and the whole structure is slightly complex.
disclosure of Invention
The utility model aims to solve the technical problem that the shortcoming of current two-dimentional magneto-optical trap optical device has been overcome, a novel two-dimentional magneto-optical trap's optical device that reasonable in design, simple structure, work efficiency are high is provided.
The technical scheme for solving the technical problems is as follows: a two-dimensional magneto-optical trap cavity is arranged in the middle of the mounting platform, an integrated collimating mirror A is arranged on the mounting platform on the right front side of the two-dimensional magneto-optical trap cavity, light spots emitted by the integrated collimating mirror A penetrate through rectangular windows on the front side and the rear side of the two-dimensional magneto-optical trap cavity and irradiate a first 45-degree high-reflection mirror group A arranged on the mounting platform on the rear side of the two-dimensional magneto-optical trap cavity, the first 45-degree high-reflection mirror group A consists of two 45-degree high-reflection mirrors with an included angle of 90 degrees, and a quarter wave plate A and a zero-degree high-reflection mirror A are sequentially arranged on the mounting platform in the reflected light emitting direction of the first 45-degree high-reflection mirror group A on the;
An integrated collimating mirror B is arranged on a mounting platform positioned at the lower right of the two-dimensional magneto-optical trap cavity, light spots emitted by the integrated collimating mirror B penetrate through rectangular windows at the upper side and the lower side of the two-dimensional magneto-optical trap cavity and irradiate a first 45-degree high-reflection mirror group B arranged on the mounting platform positioned above the two-dimensional magneto-optical trap cavity, and a quarter wave plate B and a zero-degree high-reflection mirror B are sequentially arranged on the mounting platform in the reflected light emitting direction of the first 45-degree high-reflection mirror group B positioned below the two-dimensional magneto-optical trap cavity; the integrated collimating lens B, the first 45-degree high reflecting lens group B, the quarter wave plate B and the zero-degree high reflecting lens B are correspondingly equal to the integrated collimating lens A, the first 45-degree high reflecting lens group A, the quarter wave plate A and the zero-degree high reflecting lens A.
The integrated collimating lens A is structurally characterized in that an end cover at one end of a lens barrel is provided with an optical fiber connector, and a first broadband polarization beam splitter prism, a half wave plate, a second broadband polarization beam splitter prism, a double-cemented lens and a quarter wave plate are sequentially arranged in the lens barrel along the transmission direction of light.
As a preferred technical scheme, a second 45-degree high-reflection mirror group a is arranged on a first 45-degree high-reflection mirror group a reflected light emergent direction mounting platform positioned at the front side of the two-dimensional magneto-optical trap cavity, a quarter wave plate a and a zero-degree high-reflection mirror a are sequentially arranged on the second 45-degree high-reflection mirror group a reflected light emergent direction mounting platform, the quarter wave plate a and the zero-degree high-reflection mirror a are positioned at the rear side of the two-dimensional magneto-optical trap cavity, and the first 45-degree high-reflection mirror group a and the second 45-degree high-reflection mirror group a have the same structure.
As a preferred technical scheme, a second 45-degree high-reflection mirror group B is arranged on a first 45-degree high-reflection mirror group B reflected light emitting direction mounting platform below the two-dimensional magneto-optical trap cavity, a quarter wave plate B and a zero-degree high-reflection mirror B are sequentially arranged on the second 45-degree high-reflection mirror group B reflected light emitting direction mounting platform, the quarter wave plate B and the zero-degree high-reflection mirror B are located above the two-dimensional magneto-optical trap cavity, and the first 45-degree high-reflection mirror group B and the second 45-degree high-reflection mirror group B have the same structure.
As a preferable technical solution, the distance between the first broadband polarization splitting prism and the optical fiber connector is 20mm, the distance between the first broadband polarization splitting prism and the half-wave plate is 2mm, the distance between the half-wave plate and the second broadband polarization splitting prism is 7mm, the distance between the second broadband polarization splitting prism and the double cemented lens is 100-120 mm, and the distance between the double cemented lens and the quarter-wave plate is 5 mm.
As a preferable technical scheme, the incident surface and the bonding surface of the double-bonded lens are convex surfaces which are convex towards the light incident direction, the emergent surface is convex surfaces which are convex towards the light emergent direction, the curvature radius of the incident surface is 124-150 mm, the curvature radius of the bonding surface is 31-40 mm, the curvature radius of the emergent surface is-35-60 mm, and the incident surface and the emergent surface of the double-bonded lens are both plated with antireflection films.
As a preferred technical scheme, the width of an incident window of the two-dimensional magneto-optical trap cavity is 1.1-1.2 times of the diameter of an emergent light spot of the integrated collimating mirror A, the length of the incident window of the two-dimensional magneto-optical trap cavity is more than or equal to 2 times of the diameter N of the emergent light spot of the integrated collimating mirror, and N is a positive integer.
As a preferable technical scheme, the diameter of the zero-degree high-reflection mirror A is 1.1-1.3 times of the diameter of the emergent light spot of the integrated collimating mirror A.
As a preferable technical scheme, the diameter of the 45-degree high-reflection mirror is 1.4-1.5 times of the diameter of the emergent light spot of the integrated collimating mirror A.
The utility model has the advantages as follows:
1. Compared with the prior art, the novel two-dimensional magneto-optical trap optical-mechanical structure does not use a polarization splitting prism and reduces the use of a quarter wave plate, avoids the influence of external temperature change on the whole device, and improves the stability of the whole device.
2. Compared with the prior art, the utility model the quantity of device reduces, but can reach the function the same with prior art and produce the atomic beam at a slow speed promptly, has simple structure, compactness, advantage that area is little.
3. The utility model discloses an integration collimating mirror A and integration collimating mirror B are different with the integration collimating mirror structure that current two-dimentional magneto-optical trap used, along the emitting direction of light the utility model discloses last device is the quarter wave plate in integration collimating mirror A and integration collimating mirror B's the lens cone, and last device is the half wave plate in the current integration collimating mirror lens cone.
4. The utility model discloses an add the high mirror group of 45 degrees, increased cooling light standing wave field, prolonged atom and cooling light standing wave field contact route, the speed that makes the slow speed atomic beam of formation is slower, has improved work efficiency.
Drawings
Fig. 1 is a schematic diagram of an optical path in one dimension in the prior art.
Fig. 2 is a schematic diagram of the structure principle of the embodiment 1 of the present invention.
Fig. 3 is a schematic structural diagram of embodiment 2 of the present invention.
fig. 4 is a schematic structural diagram of the integrated collimating mirror A8 of the present invention.
Detailed Description
The present invention will be described in further detail with reference to the drawings and examples, but the present invention is not limited to the following embodiments.
Example 1
In fig. 2, the optical mechanical device of the novel two-dimensional magneto-optical trap of this embodiment is formed by connecting a two-dimensional magneto-optical trap cavity 1, a first 45-degree high-reflection mirror group B2, a first 45-degree high-reflection mirror group A3, an integrated collimating mirror B4, a mounting platform 5, a zero-degree high-reflection mirror B6, a quarter-wave plate B7, an integrated collimating mirror A8, a zero-degree high-reflection mirror a9, and a quarter-wave plate a 10.
The middle part of the mounting platform 5 is provided with a two-dimensional magneto-optical trap cavity 1, the two-dimensional magneto-optical trap cavity 1 contains a product which is sold on the market and has gradient magnetic field distribution, one end of the two-dimensional magneto-optical trap cavity 1 is provided with an atom steam inlet, the other end is provided with a slow atom beam outlet, the mounting platform 5 which is positioned at the right front side of the two-dimensional magneto-optical trap cavity 1 is provided with an integrated collimating lens A8, a light spot emitted by the integrated collimating lens A8 passes through rectangular windows at the front side and the rear side of the two-dimensional magneto-optical trap cavity 1 and irradiates on a first 45-degree high-reflection lens group A3 which is arranged on the mounting platform 5 which is positioned at the rear side of the two-dimensional magneto-optical trap cavity 1, the width of an incident window of the two-dimensional magneto-optical trap cavity 1 is 1.15 times of the diameter of an emergent light spot of the integrated collimating lens A8, the length is 2 times of the diameter of the emergent light spot of the integrated collimating lens A8, the first 45-, a quarter wave plate A10 and a zero-degree high-reflection mirror A9 are sequentially arranged on a first 45-degree high-reflection mirror group A3 reflected light emergent direction mounting platform 5 positioned at the front side of the two-dimensional magneto-optical trap cavity 1, and the diameter of the zero-degree high-reflection mirror A9 is 1.2 times that of an emergent light spot of an integrated collimating mirror A8; an integrated collimating mirror B4 is mounted on a mounting platform 5 positioned at the lower right of the two-dimensional magneto-optical trap cavity 1, light spots emitted by the integrated collimating mirror B4 penetrate through rectangular windows at the upper side and the lower side of the two-dimensional magneto-optical trap cavity 1 and irradiate a first 45-degree high-reflection mirror group B2 mounted on the mounting platform 5 positioned above the two-dimensional magneto-optical trap cavity 1, a quarter-wave plate B7 and a zero-degree high-reflection mirror B6 are sequentially mounted on the first 45-degree high-reflection mirror group B2 reflected light emitting direction mounting platform 5 positioned below the two-dimensional magneto-optical trap cavity 1, and the integrated collimating mirror B4, the first 45-degree high-reflection mirror B2, the quarter-wave plate B7, the zero-degree high-reflection mirror B6, the integrated collimating mirror A8, the first 45-degree high-reflection mirror group A3, the quarter-wave plate A10 and the zero-degree high-reflection mirror.
In fig. 4, the integrated collimating lens a4 of this embodiment is formed by connecting a lens barrel 4-2, an optical fiber connector 4-1, a first broadband polarization splitting prism 4-3, a half-wave plate 4-4, a second broadband polarization splitting prism 4-5, a double cemented lens 4-6, and a quarter-wave plate 4-7.
An optical fiber connector 4-1 is arranged on an end cover at one end of a lens barrel 4-2, an optical fiber is connected on the optical fiber connector 4-1, a first broadband polarization beam splitter prism 4-3, a half wave plate 4-4, a second broadband polarization beam splitter prism 4-5, a double cemented lens 4-6 and a quarter wave plate 4-7 are sequentially arranged in the lens barrel 4-2 along the transmission direction of light, the distance between the first broadband polarization beam splitter prism 4-3 and the optical fiber connector 4-1 is 20mm, the distance between the first broadband polarization beam splitter prism 4-3 and the half wave plate 4-4 is 2mm, the distance between the half wave plate 4-4 and the second broadband polarization beam splitter prism 4-5 is 7mm, the distance between the second broadband polarization beam splitter prism 4-5 and the double cemented lens 4-6 is 110mm, the distance between the double cemented lens 4-6 and the quarter-wave plate 4-7 is 5mm, the incident surface and the cemented surface of the double cemented lens 4-6 are convex surfaces protruding towards the light incident direction, the emergent surface is convex surface protruding towards the light emergent direction, the curvature radius of the incident surface is 140mm, the curvature radius of the cemented surface is 35mm, the curvature radius of the light emergent surface is-50 mm, the incident surface and the emergent surface of the double cemented lens 4-6 are both plated with antireflection film, the laser enters the lens barrel 4-2 of the integrated collimating lens A through the optical fiber and passes through the middle first broadband polarization beam splitter prism 4-3, the half-wave plate 4-4, the second broadband polarization beam splitter prism 4-5 and the double cemented lens 4-6 to generate collimation beam expanding laser required by a two-dimensional magneto-optic trap, the expanded laser light generates circularly polarized light through a quarter-wave plate 4-7 in a lens barrel 4-2.
The circularly polarized light output by the integrated collimating mirror A4 passes through the two-dimensional magnetic light trap cavity 1, then passes through the two-dimensional magnetic light trap cavity 1 again after being reflected by the first 45-degree high-reflection mirror group A3, then passes through the quarter-wave plate A10, finally returns along the reverse direction of the original path after being reflected by the 0-degree high-reflection mirror group A to form a cooling light standing wave field in the one-dimensional direction by interacting with the atom steam, the circularly polarized light output by the integrated collimating mirror B passes through the two-dimensional magnetic light trap cavity 1, then passes through the two-dimensional magnetic light trap cavity 1 again after being reflected by the first 45-degree high-reflection mirror group B2, then passes through the quarter-wave plate B7, finally returns along the reverse direction of the original path after being reflected by the 0-degree high-reflection mirror B to form a cooling light standing wave field in the vertical dimension direction by interacting with the atom steam, when the atom enters from the atom steam inlet of the two-dimensional magnetic light trap cavity 1, the atom, pre-cooling and decelerating in two-dimensional direction, and finally allowing the formed slow atom beam to enter the three-dimensional magneto-optical trap through a slow atom beam outlet.
example 2
In fig. 3, the two-dimensional magneto-optical trap optical-mechanical device of the present embodiment is formed by connecting a mounting platform 5, a two-dimensional magneto-optical trap cavity 1, an integrated collimating mirror A8, a first 45-degree high-reflection mirror group A3, a second 45-degree high-reflection mirror group a12, a quarter-wave plate a10, a zero-degree high-reflection mirror a9, an integrated collimating mirror B4, a first 45-degree high-reflection mirror group B2, a second 45-degree high-reflection mirror group B11, a quarter-wave plate B7, and a zero-degree high-reflection mirror B6.
The middle part of the mounting platform 5 is provided with a two-dimensional magneto-optical trap cavity 1, the two-dimensional magneto-optical trap cavity 1 contains a product which is sold on the market and has gradient magnetic field distribution, one end of the two-dimensional magneto-optical trap cavity 1 is provided with an atom steam inlet, the other end is provided with a slow atom beam outlet, the mounting platform 5 which is positioned at the right front side of the two-dimensional magneto-optical trap cavity 1 is provided with an integrated collimating lens A8, a light spot emitted by the integrated collimating lens A8 passes through rectangular windows at the front side and the rear side of the two-dimensional magneto-optical trap cavity 1 and irradiates on a first 45-degree high-reflection lens group A3 which is arranged on the mounting platform 5 which is positioned at the rear side of the two-dimensional magneto-optical trap cavity 1, the width of an incident window of the two-dimensional magneto-optical trap cavity 1 is 1.15 times of the diameter of an emergent light spot of the integrated collimating lens A8, the length is 2 times of the diameter of the emergent light spot of the integrated collimating lens A8, the first 45-, a second 45-degree high-reflection mirror group A12 is arranged on a first 45-degree high-reflection mirror group A3 reflected light emergent direction mounting platform 5 positioned at the front side of the two-dimensional magnetic-optical trap cavity 1, a quarter-wave plate A10 and a zero-degree high-reflection mirror A9 are sequentially arranged on the second 45-degree high-reflection mirror group A12 reflected light emergent direction mounting platform 5, the quarter-wave plate A10 and the zero-degree high-reflection mirror A9 are positioned at the rear side of the two-dimensional magnetic-optical trap cavity 1, and the diameter of the zero-degree high-reflection mirror A9 is 1.2 times that of an emergent light spot of the integrated collimating mirror A8; an integrated collimating mirror B4 is mounted on a mounting platform 5 positioned at the lower right of the two-dimensional magneto-optical trap cavity 1, light spots emitted by the integrated collimating mirror B4 penetrate through rectangular windows at the upper and lower sides of the two-dimensional magneto-optical trap cavity 1 and irradiate a first 45-degree high-reflection mirror group B2 mounted on the mounting platform 5 positioned above the two-dimensional magneto-optical trap cavity 1, a second 45-degree high-reflection mirror group B11 is mounted on the first 45-degree high-reflection mirror group B2 reflected light emitting direction mounting platform 5 positioned below the two-dimensional magneto-optical trap cavity 1, a quarter-wave plate B7 and a zero-degree high-reflection mirror B6 are sequentially mounted on the second 45-degree high-reflection mirror group B11 reflected light emitting direction mounting platform 5, a quarter-wave plate B7 and a zero-degree high-reflection mirror B6 are positioned above the two-dimensional magneto-optical trap cavity 1, and a second 45-degree high-reflection mirror group A12, a first 45-degree high-reflection mirror group B2 and a second 45-degree high-reflection mirror group B63. The other components and the connection relationship of the components are the same as those in embodiment 1.
Example 3
In embodiments 1 and 2, the incident surface and the cemented surface of the double cemented lens 4-6 of the integrated collimating lens a4 are convex surfaces protruding towards the light incident direction, the emitting surface is convex surface protruding towards the light emitting direction, the radius of curvature of the incident surface is 124mm, the radius of curvature of the cemented surface is 31mm, the radius of curvature of the light emitting surface is-35 mm, and the incident surface and the emitting surface of the double cemented lens 4-6 are both plated with antireflection films; the width of an incident window of the two-dimensional magneto-optical trap cavity 1 is 1.1 times of the diameter of an emergent light spot of the integrated collimating lens A8, the length of the incident window is 3 times of the diameter of the emergent light spot of the integrated collimating lens A8, the diameter of the zero-degree high-reflection lens A9 is 1.1 times of the diameter of the emergent light spot of the integrated collimating lens A8, and the diameter of the 45-degree high-reflection lens is 1.4 times of the diameter of the emergent light spot of the integrated collimating lens A8. Other components and the connection relationship of the components are the same as those of the corresponding embodiments.
Example 4
In embodiments 1 and 2, the incident surface and the cemented surface of the double cemented lens 4-6 of the integrated collimating lens a4 are convex surfaces protruding towards the light incident direction, the exit surface is convex surface protruding towards the light exit direction, the radius of curvature of the incident surface is 150mm, the radius of curvature of the cemented surface is 40mm, the radius of curvature of the light exit surface is-60 mm, and the incident surface and the exit surface of the double cemented lens 4-6 are both plated with antireflection films; the width of an incident window of the two-dimensional magneto-optical trap cavity 1 is 1.2 times of the diameter of an emergent light spot of the integrated collimating lens A8, the length of the incident window is 5 times of the diameter of the emergent light spot of the integrated collimating lens A8, the diameter of the zero-degree high-reflection lens A9 is 1.3 times of the diameter of the emergent light spot of the integrated collimating lens A8, and the diameter of the 45-degree high-reflection lens is 1.5 times of the diameter of the emergent light spot of the integrated collimating lens A8. Other components and the connection relationship of the components are the same as those of the corresponding embodiments.

Claims (8)

1. The utility model provides a novel ray apparatus of two dimension magneto-optical trap which characterized in that: a two-dimensional magneto-optical trap cavity (1) is arranged in the middle of the mounting platform (5), an integrated collimating mirror A (8) is arranged on the right front side mounting platform (5) positioned in the two-dimensional magneto-optical trap cavity (1), light spots emitted by the integrated collimating mirror A (8) penetrate through rectangular windows on the front side and the rear side of the two-dimensional magneto-optical trap cavity (1) and irradiate a first 45-degree high-reflection mirror group A (3) arranged on the mounting platform (5) on the rear side of the two-dimensional magneto-optical trap cavity (1), the first 45-degree high-reflection mirror group A (3) is composed of two 45-degree high-reflection mirrors with an included angle of 90 degrees, and a quarter wave plate A (10) and a zero-degree high-reflection mirror A (9) are sequentially arranged on the reflected light emitting direction mounting platform (5) of the first 45-degree high-reflection mirror group A (3) positioned on the front side;
An integrated collimating mirror B (4) is arranged on a mounting platform (5) positioned at the lower right of the two-dimensional magneto-optical trap cavity (1), light spots emitted by the integrated collimating mirror B (4) penetrate through rectangular windows at the upper side and the lower side of the two-dimensional magneto-optical trap cavity (1) and irradiate a first 45-degree high-reflection mirror group B (2) arranged on the mounting platform (5) positioned above the two-dimensional magneto-optical trap cavity (1), and a quarter-wave plate B (7) and a zero-degree high-reflection mirror B (6) are sequentially arranged on the mounting platform (5) in the direction of reflected light emission of the first 45-degree high-reflection mirror group B (2) positioned below the two-dimensional magneto-optical trap cavity (1); the integrated collimating lens B (4), the first 45-degree high-reflection lens group B (2), the quarter-wave plate B (7) and the zero-degree high-reflection lens B (6) are correspondingly equal to the integrated collimating lens A (8), the first 45-degree high-reflection lens group A (3), the quarter-wave plate A (10) and the zero-degree high-reflection lens A (9);
The integrated collimating lens B (4) is structurally characterized in that an end cover at one end of a lens barrel (4-2) is provided with an optical fiber connector (4-1), and a first broadband polarization splitting prism (4-3), a half wave plate (4-4), a second broadband polarization splitting prism (4-5), a double cemented lens (4-6) and a quarter wave plate (4-7) are sequentially arranged in the lens barrel (4-2) along the transmission direction of light.
2. The new optomechanical device of two-dimensional magneto-optical trap as claimed in claim 1, wherein: be located two-dimentional magneto-optical trap chamber (1) front side first 45 degrees high reflection mirror group A (3) reverberation exit direction mounting platform (5) on be provided with the high reflection mirror group A (12) of second 45 degrees, set gradually quarter wave plate A (10) and the high reflection mirror A (9) of zero degree on the high reflection mirror group A (12) reverberation exit direction mounting platform (5) of second 45 degrees, quarter wave plate A (10) and the high reflection mirror A (9) of zero degree are located two-dimentional magneto-optical trap chamber (1) rear side, the high reflection mirror group A (3) of first 45 degrees be the same with the high reflection mirror group A (12) structure of second 45 degrees.
3. The new optomechanical device of two-dimensional magneto-optical trap as claimed in claim 1, wherein: be located two-dimentional magneto-optical trap chamber (1) below first 45 degrees high reflection mirror group B (2) reverberation exit direction mounting platform (5) on be provided with second 45 degrees high reflection mirror group B (11), second 45 degrees high reflection mirror group B (11) reverberation exit direction mounting platform (5) on have set gradually quarter wave plate B (7) and zero degree high reflection mirror B (6), quarter wave plate B (7) and zero degree high reflection mirror B (6) are located two-dimentional magneto-optical trap chamber (1) top, first 45 degrees high reflection mirror group B (2) and second 45 degrees high reflection mirror group B (11) the structure the same.
4. The new optomechanical device of two-dimensional magneto-optical trap as claimed in claim 1, wherein: the distance between the first broadband polarization beam splitter prism (4-3) and the optical fiber connector (4-1) is 20mm, the distance between the first broadband polarization beam splitter prism (4-3) and the half wave plate (4-4) is 2mm, the distance between the half wave plate (4-4) and the second broadband polarization beam splitter prism (4-5) is 7mm, the distance between the second broadband polarization beam splitter prism (4-5) and the double cemented lens (4-6) is 100-120 mm, and the distance between the double cemented lens (4-6) and the quarter wave plate (4-7) is 5 mm.
5. The new optomechanical device of two-dimensional magneto-optical trap as claimed in claim 1, wherein: the incident surface and the bonding surface of the double-bonded lens (4-6) are convex surfaces protruding towards the light incident direction, the emergent surface is convex surfaces protruding towards the light emergent direction, the curvature radius of the incident surface is 124-150 mm, the curvature radius of the bonding surface is 31-40 mm, the curvature radius of the emergent surface is-35-60 mm, and the incident surface and the emergent surface of the double-bonded lens (4-6) are both plated with antireflection films.
6. A novel optomechanical device of two-dimensional magneto-optical trap as claimed in claim 1, 2 or 3, wherein: the width of an incident window of the two-dimensional magneto-optical trap cavity (1) is 1.1-1.2 times of the diameter of an emergent light spot of the integrated collimating mirror A (8), the length of the incident window is more than or equal to 2 times of the diameter N of the emergent light spot of the integrated collimating mirror, and N is a positive integer.
7. A novel optomechanical device of two-dimensional magneto-optical trap as claimed in claim 1, 2 or 3, wherein: the diameter of the zero-degree high-reflection mirror A (9) is 1.1-1.3 times of the diameter of the emergent light spot of the integrated collimating mirror A (8).
8. A novel optomechanical device of two-dimensional magneto-optical trap as claimed in claim 1, 2 or 3, wherein: the diameter of the 45-degree high-reflection mirror is 1.4-1.5 times of the diameter of the emergent light spot of the integrated collimating mirror A (8).
CN201920425605.3U 2019-03-29 2019-03-29 Novel optical machine device of two-dimensional magneto-optical trap Expired - Fee Related CN209803572U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201920425605.3U CN209803572U (en) 2019-03-29 2019-03-29 Novel optical machine device of two-dimensional magneto-optical trap

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201920425605.3U CN209803572U (en) 2019-03-29 2019-03-29 Novel optical machine device of two-dimensional magneto-optical trap

Publications (1)

Publication Number Publication Date
CN209803572U true CN209803572U (en) 2019-12-17

Family

ID=68827280

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201920425605.3U Expired - Fee Related CN209803572U (en) 2019-03-29 2019-03-29 Novel optical machine device of two-dimensional magneto-optical trap

Country Status (1)

Country Link
CN (1) CN209803572U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109884872A (en) * 2019-03-29 2019-06-14 中国科学院国家授时中心 The optical mechanical apparatus of New Two Dimensional Magneto-Optical Trap

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109884872A (en) * 2019-03-29 2019-06-14 中国科学院国家授时中心 The optical mechanical apparatus of New Two Dimensional Magneto-Optical Trap
CN109884872B (en) * 2019-03-29 2024-04-26 中国科学院国家授时中心 Optical machine device of two-dimensional magneto-optical trap

Similar Documents

Publication Publication Date Title
CN110233417B (en) Device for improving diamond Raman laser efficiency
CN202267786U (en) Reflectivity-variable laser beam splitter
CN203838377U (en) Parallel transmission optical module coupling/light-splitting structure
US4178561A (en) Scanning arrangements for optical frequency converters
CN209803572U (en) Novel optical machine device of two-dimensional magneto-optical trap
CN211955982U (en) High-precision continuously adjustable stable output laser power attenuation device
CN111399218A (en) Laser radar beam scanning system based on polarization grating
US3442591A (en) Apparatus for measuring the raman effect of samples of infinitesimal quantities
CN111579099B (en) Compact cold atom interference information acquisition device
CN101369015A (en) Light splitting apparatus of wind detection laser radar based on dual-edge detection
CN109884872B (en) Optical machine device of two-dimensional magneto-optical trap
CN108627983B (en) Laser beam combining system and beam combining method thereof
CN206833168U (en) Collimator and extender spot diameter converting means
CN212781684U (en) Holographic projection recording system
CN110098559A (en) A kind of interior device and method collimated of semiconductor laser shell
CN100412969C (en) Optical system and optical recording/reproducing device using the same
CN217087125U (en) Narrow pulse width laser with high repetition frequency and high beam quality
CN117013356A (en) Semiconductor laser assembly
US3366892A (en) Solid state laser mode selection means
CN116559836B (en) Acousto-optic deflection module based on diffusion sheet beam expansion, photoelectric device and electronic equipment
CN203551897U (en) Kilowatt collimation type isolator
CN116560155B (en) Acousto-optic deflection module based on superlens collimation, distance measuring device and electronic equipment
CN116559837B (en) Acousto-optic deflection module based on superlens collimation, photoelectric device and electronic equipment
CN116560156B (en) Acousto-optic deflection module based on cylindrical lens collimation, distance measuring device and electronic equipment
CN211905854U (en) Laser radar beam scanning system based on polarization grating

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20191217