Apparatus for detecting a photon pulse

• US 6,049,079 A
• Filed: 10/20/1997
• Issued: 04/11/2000
• Est. Priority Date: 04/21/1995
• Status: Expired due to Fees

• Current Assignee: Seed Capital Investments-2 B.V., Stichting voor Fundamenteel Onderzoek der Materie
• Original Assignee: Stichting voor Fundamenteel Onderzoek der Materie
• Inventors: Lankhuijzen, Marcelis Dominicus, Noordam, Lambertus Dominicus
• Primary Examiner(s): Westin, Edward P.
• Assistant Examiner(s): HANIG, RICHARD E
• Application Number:
  US08/945,080
• Time in Patent Office: 904 Days
• Field of Search: 250/338.1, 250/339.05, 250/374, 250/379, 250/214 VT, 348/215, 359/333
• US Class Current: 250/338.1
• CPC Class Codes: G04F 13/026 Measuring duration of ultra-short light pulses, e.g. in the pico-second range; particular detecting devices therefor photometry, radiation pyrometry G01J1/00, G01J5/00; non-linear optics G02F1/35
• CPC Class Codes: H01J 31/502 with means to interrupt the beam, e.g. shutter for high speed photography circuits using electron-beam shutters G03B27/725
• CPC Class Codes: H01J 47/00 Tubes for determining the presence, intensity, density or energy of radiation or particles discharge tubes using igniting by associated radioactive materials or fillings, e.g. current stabilising tubes H01J17/32 ; photoelectric discharge tubes not involving the ionisation of a gas H01J40/00 ; discharge tubes for measuring the pressure, partial pressure of introduced gas or for detecting presence of gas H01J41/02; ionisation chambers using a solid dielectric G01T3/008

Abstract

Streak camera whereof the pulse converter for converting a photon pulse for detecting into an electron stream comprises a gaseous medium. A streak camera for a photon pulse in the far-infrared region is provided with a laser source to bring particles in the medium into a Rydberg state, in a streak camera for an X-ray pulse the medium contains particles for bringing into an Auger state, and additional deflection plates are provided for separating a primary electron stream from a secondary electron stream.

Claims

1. Apparatus for detecting a photon pulse as a function of time, comprising a pulse converter for converting a photon pulse to be detected into an electron stream, first deflection means for deflecting the electron stream as a function of time and a position-sensitive detector for determining the deflection of the electron stream, characterized in that the pulse converter comprises a gaseous medium in order to absorb the photon pulse for detecting and to emit the electron stream.

2. Apparatus as claimed in claim 1, wherein the photon pulse lies in the far-infrared region, characterized in that the apparatus is provided with excitation means for bringing particles into an excited electron state and the gaseous medium contains particles to be brought into the said excited electron state in order to absorb the photon pulse and to emit the electron stream.

4. Apparatus as claimed in claim 2, characterized in that the excited electron state is a Rydberg state.

5. Apparatus as claimed in claim 2, characterized by an evaporation oven for bringing into gaseous state the particles for bringing into an excited electron state.

6. Apparatus as claimed in claim 2, characterized in that the particles are alkali metal atoms.

7. Apparatus as claimed in claim 6, characterized in that the alkali metal atoms comprise one of the elements Rb (rubidium) or Cs (caesium).

8. Apparatus as claimed in claim 2, characterized in that the excitation means comprise a laser light source.

9. Apparatus as claimed in claim 8, characterized in that the laser light source is a dye laser pumped with an Nd:

YAG(neodymium;

yttrium-aluminium garnet) laser.

10. Apparatus as claimed in claim 8, characterized in that the laser light source is a diode laser.

11. Apparatus as claimed in claim 1, wherein the photon pulse is an X-ray pulse, characterized in that the gaseous medium contains particles to be brought into an Auger state in order to absorb the photon pulse and to emit a primary electron stream with a determined primary electron energy and to emit, in an Auger state, a secondary electron stream with a determined secondary electron energy which differs from the primary electron energy, and second deflection means are provided for deflecting the primary and secondary electron stream in a direction differing from that of the deflection by the first deflection means, in a manner such that the primary electron stream is separated from the secondary electron stream and substantially only the deflection of the second electron stream is determined with the position-sensitive detector.

12. Apparatus as claimed in claim 11, characterized in that the second deflection means are provided to deflect the primary and secondary electron stream in a direction substantially perpendicular to the direction of the deflection by the first deflection means.

13. Apparatus as claimed in claim 11, characterized in that the particles for emitting the secondary electron stream in an Auger state are Ne (neon) atoms.

14. Apparatus as claimed in claim 1, characterized in that there is a first deflection means present at a location where the electrons for deflecting by said first deflection means emitted at a determined point in time by the gaseous medium arrive simultaneously.

15. Apparatus as claimed in claim 1, characterized in that there is a first deflection means present at a location between the pulse convertor and the position at which the electrons for deflecting by said first deflection means emitted at a determined point in time by the gaseous medium arrive simultaneously.

3. Apparatus for detecting a photon pulse in the infrared region as a function of time, comprising a pulse converter for converting a photon pulse for detecting into an electron stream and a detector for this electron stream, characterized in that the apparatus is provided with excitation means for bringing particles into an excited electron state and the pulse converter comprises a gaseous medium with particles for bringing into this excited electron state in order to absorb the photon pulse and to emit the electron stream.