EP1230564A1 - X-ray beam position monitor - Google Patents

X-ray beam position monitor

Info

Publication number
EP1230564A1
EP1230564A1 EP00966329A EP00966329A EP1230564A1 EP 1230564 A1 EP1230564 A1 EP 1230564A1 EP 00966329 A EP00966329 A EP 00966329A EP 00966329 A EP00966329 A EP 00966329A EP 1230564 A1 EP1230564 A1 EP 1230564A1
Authority
EP
European Patent Office
Prior art keywords
ray beam
electrodes
plane
electrode
series
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.)
Withdrawn
Application number
EP00966329A
Other languages
German (de)
English (en)
French (fr)
Inventor
Ulrich Wolfgang Arndt
Martin Paul Kyte
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.)
Medical Research Council
Original Assignee
Medical Research Council
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 Medical Research Council filed Critical Medical Research Council
Publication of EP1230564A1 publication Critical patent/EP1230564A1/en
Withdrawn legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/29Measurement performed on radiation beams, e.g. position or section of the beam; Measurement of spatial distribution of radiation
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/26Measuring radiation intensity with resistance detectors

Definitions

  • This invention relates to X-ray beam position monitors and represents a development of the invention disclosed in the applicants' co-pending UK Patent Application No 9913615.2.
  • the aim of the invention is to provide monitoring of at least the rotational positions of the X-ray beam, and preferably both translational and rotational positions.
  • an X-ray beam position monitor comprises a first electrode assembly for detecting the rotational position of the X-ray beam about an axis orthogonal to one plane, the first electrode assembly comprising a first series of three collection electrodes and a first biasing electrode, a second electrode assembly for detecting the rotational position of the X-ray beam about another axis orthogonal to another plane transverse to said one plane, the second electrode assembly comprising a second series of three collection electrodes and a second biasing electrode, means for applying a bias voltage to the biasing electrodes and signal processing means for processing electrical signals which are generated at the collection electrodes and deriving therefrom signals which are representative of the rotational position of the X-ray beam about said axes.
  • the three collection electrodes of the first series are preferably constituted by an intermediate electrode in the shape of a parallelogram adjacent to which are two end electrodes each triangular in shape, the series of the three collection electrodes preferably having in overall outline a generally rectangular shape.
  • the processing means are preferably operative to sum the signals from the end electrodes and subtract therefrom the signal from the intermediate electrode, in order to derive a signal representative of the rotational position of the X-ray beam in said one plane.
  • This latter signal may be normalised by dividing it by the sum of the signals from the three electrodes.
  • the monitor may also detect the translational position of the X-ray beam in said one plane, in which case the signal processing means are additionally operative to obtain the difference between the signals from the two end electrodes, in order to derive a signal representative of the translational position of the X-ray beam in said one plane. This latter may be normalised by dividing it by the signal from the intermediate electrode.
  • the three collection electrodes of the second series are preferably constituted by a second intermediate electrode in the shape of a parallelogram adjacent to which are two second end electrodes each triangular in shape, the series of the three collection electrodes of the second series preferably having in overall outline a generally rectangular shape.
  • the processing means are preferably operative to sum the signals from the second end electrodes and subtract therefrom the signal from the second intermediate electrode, in order to derive a signal representative of the rotational position of the X-ray beam in said another plane.
  • the monitor may also detect the translational position of the X-ray beam in said another plane, in which case the signal processing means are additionally operative to obtain the difference between the signals from the two second end electrodes, in order to derive a signal representative of the translational position of the X-ray beam in said another plane.
  • the first electrode assembly and the second electrode assembly may be positioned at substantially the same axial position along the direction of propagation of the X-ray beam, in which case the means for applying the bias voltage include switching means for applying the bias voltage to the first biasing electrode or the second biasing electrode.
  • the first electrode assembly and the second electrode assembly are not at the same axial position along the direction of propagation of the X-ray beam.
  • the electrodes of the first assembly are preferably orthogonal to the electrodes of the second assembly, so that said one plane and said other plane are mutually orthogonal.
  • the first and second electrode assemblies When the first and second electrode assemblies are placed at substantially the same position along the direction of propagation of the X-ray beam, the first and second electrode assemblies preferably constitute the four walls of a square-section tunnel-like structure through which the X-ray beam is propagated.
  • the X-ray beam position sensor preferably acts as a null-seeking device, the beam being centred (in both translational and rotational senses) by means of adjustments in the two planes of positioning, until the electrical signals are representative of a centred position of the X-ray beam.
  • This adjustment can be simultaneous when the first and second electrode assemblies are axially spaced, but is sequential in the two planes of positioning when the first and second electrode assemblies are at the same axial position. Adjustment may be achieved by applying a centring movement to the beam, to the assembly or to a combination of both beam and assembly.
  • Figure 1 is a view showing the structure of collection and bias electrodes in the first embodiment.
  • Figure 2 is a view showing three collection electrodes of the first embodiment.
  • Figure 3 shows the electrical circuitry of the embodiment of Figure 1 .
  • Figure 4 is a view showing the structure of collection and bias electrodes of the second embodiment.
  • the sensor comprises a first electrode assembly comprising a first series of three collection electrodes la, lb, lc printed on a first anode board 2, and a first biasing electrode 3 printed on a first cathode board 4.
  • the anode and cathode boards 2 and 4 occupy vertically spaced horizontal planes with the first series of collection electrodes la, lb, lc facing the first biasing electrode 3.
  • the first biasing electrode 3 is rectangular in shape, the first series of three collection electrodes la, lb, lc, having, in overall outline, a similar rectangular shape which is divided by two angled but mutually parallel lines of separation so that the electrode lb defines an intermediate electrode in the shape of a parallelogram and the two electrodes la and lc are end electrodes each in the shape of a right-angled triangle.
  • the pair of boards 2 and 8 are separated by a short distance from the pair of boards 3 and 6.
  • the first anode board 2 and its three collection electrodes la, lb and lc are shown in Figure 2.
  • Also shown diagrammatically in Figure 2 are the respective electrical connections to the three electrodes la, lb and lc.
  • the second electrode assembly comprises a second series of three collection electrodes 5a, 5b, 5c printed on a second anode board 6, and a second biasing electrode 7 printed on a second cathode board 8.
  • the second anode and cathode boards occupy horizontally spaced vertical planes, with the second series of collection electrodes 5a, 5b, 5c facing the second biasing electrode 7.
  • the second biasing electrode 7 is rectangular in shape, the second series of three collection electrodes 5a, 5b, 5c having, in overall outline, a similar rectangular shape which is divided by two angled but mutually parallel lines of separation so that the electrode 5b defines an intermediate electrode in the shape of a parallelogram and the two end electrodes 5a, 5b are in the shape of right-angled triangles.
  • Each electrode la, lb, lc, 5a, 5b, 5c, 3 and 7 is formed by an area of copper deposited on the appropriate board.
  • the first and second electrode assemblies are positioned at the same axial position along the direction of propagation of the X-ray beam, the centred direction of which is indicated at 9 in Figure 1.
  • the first and second electrode assemblies thus form a tunnel like structure of square cross-sectional shape, through which the X-ray beam is propagated.
  • each board is a rectangle 8mm wide by 36mm long, with a spacing of 10mm between anode and cathode.
  • the air-filled tunnel-like structure is 36mm long and has a square cross-sectional shape with an edge dimension of 10mm. This structure fits within a 25mm diameter tube, thus providing a compact arrangement.
  • the two cathode or biasing electrodes 3, 7 are connected to a double pole switch 10, in one position of which (illustrated in Figure 3) the electrode 7 is grounded and the electrode 3 is connected to a -300 volt source 12, and in the other position of which the electrode 7 is connected to the -300 volt source 12 and the electrode 3 is grounded.
  • Figure 3 is diagrammatic because there is no transverse plane which would show all six of these electrodes.
  • the three collection electrodes la, lb, lc are respectively electrically connected to three current to voltage amplifiers 13, 14, 15 each having a respective feedback resistor 16, 17, 18 typically of 20 G ⁇ .
  • the amplifiers 13, 14, 15 have respective voltage outputs Va,, Vb, and Vc, respectively proportional to the charges collected on the electrodes la, lb and lc as a result of the ionisation produced by the X-ray beam.
  • the three collection electrodes 5a, 5b, 5c are respectively connected to three current to voltage amplifiers 19, 20, 21 each having a respective feedback resistor 23, 24, 25 of 20 G ⁇ .
  • the three amplifiers 19, 20, 21 have respective voltage outputs Va 2 , Vb 2 and Vc 2 respectively proportional to the charges collected on the electrodes 5a, 5b and 5c as a result of the ionisation produced by the X-ray beam.
  • the voltages Va, Vb, Vc are used to derive a first signal R, representative of the rotational displacement (about the central vertical axis 26) of the X-ray beam from the central axis.
  • R Va, + Vc, -Vb, Va, + Vb, + Vc,
  • R is indicative of the rotation (about the vertical axis 26) required to make the X-ray beam parallel to the central axis.
  • the denominator in the above expression for R normalises the signal.
  • the voltages Va,, Vb,, and Vc are used to derive a first signal T, representative of the translational displacement of the X-ray beam, in a horizontal plane, from the centre of the chamber.
  • T, Va, - Vc, Vb, where the denominator normalises the signal. It can be shown that T, changes from + 1 through 0 to -1 as the position of the beam moves from one long edge of the electrode through the centre to the other long edge. As a result of normalisation, the values of R, and T, are independent of the X-ray beam intensity and depend solely on the beam position.
  • the voltages Va 2 Vb 2 and Vc 2 are used to derive a second signal R 2 representative of the rotational displacement (about the transverse horizontal axis 27) of the X-ray beam from the central axis.
  • R 2 Va, + Vc, - Vb, Va 2 + Vb 2 + Vc 2
  • R 2 is indicative of the rotation (about the horizontal axis 27) required to make the beam parallel to the central axis. It can be shown that
  • the voltages Va 2 Vb 2 and Vc 2 are used to derive a second signal T 2 representative of the translational displacement of the X-ray beam (in a vertical plane, from the centre of the chamber) .
  • T 2 changes from + 1 through 0 to -1 as the position of the beam moves from one long edge of the electrode through the centre to the other long edge.
  • R 2 and T are independent of the X-ray beam intensity and depend solely on the beam position.
  • the beam is positioned so as to be maintained in its aligned central position, the alignment of the beam being carried out by sequential adjustment in the horizontal and vertical planes until R, T,, R, and T, are all 0.
  • This centring process can be carried out automatically by a central processing unit.
  • the embodiment of Figure 1 is a compact arrangement in which the first and second series of electrodes are located at the same axial position along the direction of propagation of the X-ray beam.
  • the first series of electrodes la, lb, lc, 3 are located at a different position along the direction of propagation of the X-ray beam from the second series of electrodes 5a, 5b, 5c, 7.
  • the X-ray beam passes first through the first series of electrodes and then through the second series of electrodes.
  • the signal processing for the embodiment of Figure 4 is the same as for Figure 2, but it is not necessary to use a change-over switch 10 because the bias voltage 12 can be applied to both collection electrodes simultaneously and the signals R, T, R 2 and T 2 are thus obtainable simultaneously and continuously over a chosen period of time.

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Molecular Biology (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Measurement Of Radiation (AREA)
  • X-Ray Techniques (AREA)
EP00966329A 1999-11-16 2000-10-12 X-ray beam position monitor Withdrawn EP1230564A1 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
GB9926933 1999-11-16
GB9926933A GB2356928B (en) 1999-11-16 1999-11-16 X-ray beam position monitors
PCT/GB2000/003917 WO2001036998A1 (en) 1999-11-16 2000-10-12 X-ray beam position monitors

Publications (1)

Publication Number Publication Date
EP1230564A1 true EP1230564A1 (en) 2002-08-14

Family

ID=10864504

Family Applications (1)

Application Number Title Priority Date Filing Date
EP00966329A Withdrawn EP1230564A1 (en) 1999-11-16 2000-10-12 X-ray beam position monitor

Country Status (6)

Country Link
EP (1) EP1230564A1 (ja)
JP (1) JP2003515142A (ja)
AU (1) AU767730B2 (ja)
CA (1) CA2387794A1 (ja)
GB (1) GB2356928B (ja)
WO (1) WO2001036998A1 (ja)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5379580B2 (ja) * 2008-07-16 2013-12-25 三菱電機株式会社 線量分布測定装置
JP5930628B2 (ja) * 2011-08-22 2016-06-08 株式会社日立製作所 放射線照射装置及び放射線計測方法
NL2016069A (en) * 2015-02-10 2016-09-29 Asml Netherlands Bv Radiation Sensor

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02136779A (ja) * 1988-11-16 1990-05-25 Toshiba Corp ビームモニタ
EP1207407A2 (en) * 1995-04-07 2002-05-22 Rikagaku Kenkyusho Radiation beam position monitor and position measurement method
JP3641736B2 (ja) * 1997-12-15 2005-04-27 株式会社神戸製鋼所 ビームの測定方法

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO0136998A1 *

Also Published As

Publication number Publication date
JP2003515142A (ja) 2003-04-22
WO2001036998A1 (en) 2001-05-25
AU7676800A (en) 2001-05-30
CA2387794A1 (en) 2001-05-25
GB9926933D0 (en) 2000-01-12
GB2356928A (en) 2001-06-06
AU767730B2 (en) 2003-11-20
GB2356928B (en) 2002-09-11

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