The system for analyzing multiple samples includes a plurality of portable of sample supports each for accommodating a plurality of samples thereon, and an identification mechanism for identifying each sample location on each of the plurality of sample supports. The mass spectrometer is provided for analyzing each of the plurality of samples when positioned within a sample receiving chamber, and a laser source strikes each sample with a laser pulse to desorb and ionize sample molecules. The support transport mechanism provided provides for automatically inputting and outputting each of the sample supports from the sample receiving chamber of the mass spectrometer. A vacuum lock chamber receives the sample supports and maintains at least one of the sample supports within a controlled environment while samples on another of the plurality of sample supports are being struck with laser pulses. The computer is provided for recording test data from the mass spectrometer and for controlling the operation of the system.
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0. 88. A system for obtaining mass data comprising:
a mass spectrometer comprising an ion source chamber, wherein the ion source chamber comprises
a sample receiving stage adapted to support a sample support, and
a mechanism to move the sample receiving stage;
a laser source in communication with the ion source chamber, wherein the laser source is adapted to provide a laser pulse to a sample support in the ion source chamber;
a vacuum lock chamber connected with the ion source chamber;
a sample storage chamber connected to the vacuum lock chamber, wherein the sample storage chamber comprises a sample support holder adapted to support at least one sample support; and
a sample support transfer mechanism adapted to:
(a) disassociate a first sample support from the sample receiving stage, transport the first sample support from the ion source chamber through an output port to the vacuum lock chamber and to associate the first sample support with the sample support holder; and
(b) disassociate a second sample support from the sample support holder, transport the second sample support from the vacuum lock chamber through the output port to the ion source chamber and to associate the second sample support with the sample receiving stage.
0. 75. A system for obtaining mass data comprising:
a mass spectrometer comprising an ion source chamber, wherein the ion source chamber comprises
a sample receiving stage adapted to support a sample support, and
a mechanism to move the sample receiving stage in an x direction and in a y direction perpendicular to the x direction, wherein the x direction and the y direction lie substantially in the same plane;
a laser source in optical communication with the ion source chamber, wherein the laser source is adapted to provide a laser pulse to a sample support in the ion source chamber;
a vacuum lock chamber connected with the ion source chamber, wherein the vacuum lock chamber comprises a sample support holder adapted to support more than one sample support; and
a sample support transfer mechanism adapted to:
(a) disassociate a first sample support from the sample receiving stage, transport the first sample support from the ion source chamber through an output port to the vacuum lock chamber and to associate the first sample support with the sample support holder; and
(b) disassociate a second sample support from the sample support holder, transport the second sample support from the vacuum lock chamber through the output port to the ion source chamber and to associate the second sample support with the sample receiving stage.
0. 94. A system for obtaining mass data comprising:
a mass spectrometer comprising an ion source chamber, wherein the ion source chamber comprises
a sample receiving stage adapted to support a sample support, and
a mechanism to move the sample receiving stage;
a laser source in communication with the ion source chamber, wherein the laser source is adapted to provide a laser pulse to a sample support in the ion source chamber;
a vacuum lock chamber connected with the ion source chamber;
a sample storage chamber connected to the vacuum lock chamber, wherein the sample storage chamber comprises a sample support holder adapted to support at least one sample support;
a sample support transfer mechanism adapted to:
(a) disassociate a first sample support from the sample receiving stage, transport the first sample support from the ion source chamber to the vacuum lock chamber and to associate the first sample support with the sample support holder; and
(b) disassociate a second sample support from the sample support holder, transport the second sample support from the vacuum lock chamber to the ion source chamber and to associate the second sample support with the sample receiving stage; and
means for maintaining the vacuum lock chamber and the ion source chamber in fluid communication and under a vacuum controlled environment during disassociation, transportation and association of the first and second sample supports.
0. 93. A system for obtaining mass data comprising:
a mass spectrometer comprising an ion source chamber, wherein the ion source chamber comprises
a sample receiving stage adapted to support a sample support, and
a mechanism to move the sample receiving stage in an x direction and in a y direction perpendicular to the x direction, wherein the x direction and the y direction lie substantially in the same plane;
a laser source in optical communication with the ion source chamber, wherein the laser source is adapted to provide a laser pulse to a sample support in the ion source chamber;
a vacuum lock chamber connected with the ion source chamber, wherein the vacuum lock chamber comprises a sample support holder adapted to support more than one sample support;
a sample support transfer mechanism adapted to:
(a) disassociate a first sample support from the sample receiving stage, transport the first sample support from the ion source chamber to the vacuum lock chamber and to associate the first sample support with the sample support holder; and
(b) disassociate a second sample support from the sample support holder, transport the second sample support from the vacuum lock chamber to the ion source chamber and to associate the second sample support with the sample receiving stage; and
means for maintaining the vacuum lock chamber and the ion source chamber in fluid communication and under a vacuum controlled environment during disassociation, transportation and association of the first and second sample supports.
0. 90. A method of obtaining mass data comprising the steps of:
supporting each of a plurality of samples at a fixed location on one of a plurality of sample supports;
providing an ion source chamber having a sample receiving stage adapted to support a sample support;
providing a vacuum lock chamber adapted to maintain one or more of the sample supports within a vacuum controlled environment while a sample on another of the sample supports is struck by a laser pulse,
wherein the vacuum lock chamber comprises a sample support holder adapted to receive the plurality of sample supports;
moving a first sample support associated with the sample receiving stage within the ion source chamber in an x direction and in a y direction perpendicular to the x direction;
striking with a laser pulse a desired number of the plurality of samples on the first sample support within the ion source chamber to desorb and ionize sample molecules;
disassociating the first sample support from the sample receiving stage;
transporting the first sample support from the ion source chamber to the vacuum lock chamber;
associating the first sample support with the sample support holder;
disassociating a second sample support from the sample support holder;
transporting the second sample support from the vacuum lock chamber to the ion source chamber;
associating the second sample support with the sample receiving stage;
moving the second sample support associated with the sample receiving stage within the ion source chamber in an x direction, and in a y direction perpendicular to the x direction; and
striking with a laser pulse a desired number of the plurality of samples on the second sample support within the ion source chamber to desorb and ionize sample molecules.
0. 1. A system for analyzing a plurality of samples, comprising:
a plurality of portable sample supports each having a sample receiving surface thereon for accommodating a plurality of samples each at a fixed location on each sample support;
identification means for identifying each sample location of each of the plurality of samples on each of the plurality of sample supports;
a mass spectrometer for analyzing each of the plurality of samples on each sample support, the mass spectrometer having a sample receiving chamber therein for receiving each sample support;
a laser source for striking each sample on each sample support while within the receiving chamber with a laser pulse to desorb and ionize sample molecules;
support transfer mechanism for automatically inputting and outputting each of the sample supports from the sample receiving chamber of the mass spectrometer;
a powered mechanism movable in both an x direction and a y direction perpendicular to the x direction within the sample receiving chamber for supporting a respective sample support thereon;
a vacuum lock chamber connected to the sample receiving chamber of the mass spectrometer for receiving the sample supports and for maintaining one or more of the sample supports within a vacuum controlled environment while the plurality of samples on another of the sample supports are struck by laser pulses; and
computer means for recording test data from the mass spectrometer for each of the plurality of samples on the sample supports as a function of the identification means.
0. 2. The system as defined in
a sample loading mechanism for positioning each of a plurality of liquid samples on the sample receiving surface of each of the plurality of sample supports; and
a curing chamber for drying each of the plurality of liquid samples on each of the sample supports to form a plurality of solid samples each positioned on a respective sample support.
0. 3. The system as defined in
sample support positioning means for positioning each liquid sample on the sample receiving surface of a respective sample support.
0. 4. The system as defined in
a sample preparation mechanism for automatically preparing each of the plurality of liquid samples for a deposit on a respective sample support.
0. 5. The system as defined in
0. 6. The system as defined in
valve means responsive to the computer means for automatically controlling the flow of fluids from the first and second plurality of containers.
0. 7. The system as defined in
a pump responsive to the computer means for pumping liquid samples to a respective one of the sample supports.
0. 8. The system as defined in
a drying chamber for drying liquid samples on each of the sample supports to form dried samples.
0. 9. The system as defined in
vacuum means for controlling a vacuum within the drying chamber in response to the computer means.
0. 10. The system as defined in
0. 11. The system as defined in
0. 12. The system as defined in
0. 13. The system as defined in
the identification means includes a marking on each sample support for identifying each of the plurality of samples on the sample receiving surface.
0. 14. The system as defined in
0. 15. The system as defined in
0. 16. The system as defined in
0. 17. The system as defined in
0. 18. The system as defined in
sample support identification means for identifying each of the plurality of sample supports and for inputting sample support identification information to the computer means.
0. 19. The system as defined in
a sample storage chamber for storing one or more of the plurality of sample supports; and
a powered transporter for transporting each of the plurality of sample supports from the sample storage chamber to the vacuum lock chamber.
0. 20. The system as defined in
0. 21. The system as defined in
a transport cassette for supporting a plurality of sample supports each in a preselected position within the sample storage chamber.
0. 22. The system as defined in
a transport drive mechanism for selectively positioning the transport cassette within the sample storage chamber.
0. 23. The system as defined in
0. 24. The system as defined in
0. 25. The system as defined in
a door member for selectively controlling communication between the vacuum lock chamber and the sample receiving chamber of the mass spectrometer.
0. 26. The system as defined in
a sample storage chamber for storing one or more of the plurality of sample supports; and
another door member for controlling communication between vacuum lock chamber and the sample storage chamber.
0. 27. The system as defined in
a pump for selectively evacuating the vacuum lock chamber.
0. 28. The system as defined in
each of the plurality of sample supports is moveable between the vacuum lock chamber and the receiving chamber of the mass spectrometer; and
a transporter for moving one of the plurality of samples supports within the vacuum lock chamber while the plurality of samples on another of the sample supports are being struck with laser pulses.
0. 29. The system as defined in
a powered sample support transporter for moving one or more of the plurality of sample supports within the vacuum lock chamber.
0. 30. The system as defined in
a vent valve for selectively venting the vacuum lock chamber to atmospheric pressure.
0. 31. The system as defined in
0. 32. The system as defined in
0. 33. The system as defined in
each of the plurality of sample supports includes an electromagnet secured thereto; and
power to each electromagnet is controlled in response to the computing means.
0. 34. The system as defined in
0. 35. The system as defined in
an electrically conductive block within the sample receiving chamber for receiving a respective sample support; and
one or more insulating members electrically insulating the powered positioning mechanism from the electrically conductive block.
0. 36. The system as defined in
a securing mechanism for temporarily affixing the position of a respective sample support with respect to the electrically conductive block.
0. 37. The system as defined in
an attenuator for adjusting the intensity of a laser beam output from the laser source.
0. 38. The system as defined in
0. 39. The system as defined in
0. 40. A system for analyzing a plurality of samples, comprising:
a plurality of portable sample supports each having a sample receiving surface thereon for accommodating a plurality of samples each at a fixed location on each sample support;
sample identification means for identifying each sample location of each of the plurality of samples on each of the plurality of sample supports;
support identification means for identifying each of the plurality of sample supports; and
a mass spectrometer for analyzing each of the plurality of samples on a respective one of the sample supports, the mass spectrometer having a sample receiving chamber therein for receiving a respective sample support;
a laser source for striking each sample on each sample support while within the receiving chamber with a laser pulse to desorb and ionize sample molecules;
support transfer mechanism for automatically inputting and outputting each of the sample supports from the sample receiving chamber of the mass spectrometer;
a vacuum lock chamber connected with the sample receiving chamber of the mass spectrometer for receiving each of the sample supports and for maintaining one or more of the sample supports within a vacuum controlled environment while the plurality of samples on another of the sample supports are struck by laser pulses;
a sample storage chamber for storing one or more of the plurality of sample supports;
a powered transporter for transporting each of the plurality of sample supports from the sample storage chamber to the vacuum lock chamber; and
computer means for controlling the support transfer mechanism and for receiving information from the sample identification means and the support identification means for recording test data from the mass spectrometer for each of the plurality of samples on each of the sample supports.
0. 41. The system as defined in
a sample loading mechanism for positioning each of a plurality of liquid samples on the sample receiving surface of each of the plurality of sample supports; and
a curing chamber for drying each of the plurality of liquid samples on each of the sample supports to form a plurality of solid samples each positioned on a respective sample support.
0. 42. The system as defined in
a pump responsive to the computer means for pumping liquid samples to a respective one of the sample supports.
0. 43. The system as defined in
0. 44. The system as defined in
the sample identification means includes a marking on each sample support for identifying each of the plurality of samples on the sample receiving surface.
0. 45. The system as defined in
0. 46. The system as defined in
0. 47. The system as defined in
0. 48. The system as defined in
0. 49. The system as defined in
0. 50. The system as defined in
0. 51. The system as defined in
a transport drive mechanism for selectively positioning the transport cassette within the storage chamber; and
the transport drive mechanism being powered in response to the computer means.
0. 52. The system as defined in
a door member for selectively controlling communication between the vacuum lock chamber and the sample receiving chamber of the mass spectrometer.
0. 53. The system as defined in
another door member for controlling communication between vacuum lock chamber and the sample storage chamber.
0. 54. The system as defined in
a powered sample support transporter for moving one or more of the plurality of sample supports within the vacuum lock chamber.
0. 55. The system as defined in
0. 56. The system as defined in
each of the plurality of sample supports includes an electromagnet secured thereto; and
power to each electromagnet is controlled in response to the computing means.
0. 57. The system as defined in
powered positioning mechanism for selectively positioning each of the plurality of sample supports within the sample receiving chamber.
0. 58. The system as defined in
the powered positioning mechanism is an x-y table responsive to the computing means;
an electrically conductive block within the sample receiving chamber for receiving a respective sample support; and
one or more insulating members electrically insulating the powered positioning mechanism from the electrically conductive block.
0. 59. The system as defined in
an attenuator responsive to the computer means for adjusting the intensity of a laser beam output from the laser source.
0. 60. A method of analyzing a plurality of samples within a sample receiving chamber of a mass spectrometer, the method comprising:
supporting each of a plurality of samples at a fixed location on one of a plurality of sample supports;
identifying each sample location of each of the plurality of samples on each of the plurality of sample supports;
providing a vacuum lock chamber for receiving the sample supports and for maintaining one or more of the sample supports within a vacuum controlled environment while the plurality of samples on another of the sample supports are struck by laser pulses;
automatically inputting and outputting each of the sample supports from the sample receiving chamber of the mass spectrometer to the vacuum lock chamber;
moving each sample support within the sample receiving chamber in both an x direction and a y direction perpendicular to the x direction;
striking each sample on each sample support while within the receiving chamber with a laser pulse to desorb and ionize sample molecules; and
recording test data in a computer from the mass spectrometer for each of the plurality of samples on the sample support.
0. 61. The method as defined in
positioning each of a plurality of liquid samples on the sample receiving surface of each of the plurality of sample supports; and
drying each of the plurality of liquid samples on each of the sample supports to form a plurality of solid samples each positioned on a respective sample support.
0. 62. The method as defined in
automatically preparing each of the plurality of liquid samples for deposit on a respective sample support.
0. 63. The method as defined in
arranging each of the plurality of samples in each sample support in a plurality of rows and in a plurality of columns.
0. 64. The method as defined in
marking each sample support for identifying each of the plurality of samples.
0. 65. The method as defined in
forming in excess of 80 predetermined sample positions on each of the respective sample supports.
0. 66. The method as defined in
storing one or more of the plurality of sample supports within a sample storage chamber; and
automatically transporting each of the plurality of sample supports from the sample storage chamber to the vacuum lock chamber in response to the computer.
0. 67. The method as defined in
supporting each of the plurality of sample supports at a preselected position within a transport cassette.
0. 68. The method as defined in
selectively positioning the transport cassette in response to the computer.
0. 69. The method as defined in
controlling communication from within the vacuum lock chamber to the environment exterior of the vacuum lock chamber in response to the computer.
0. 70. The method as defined in
moving a sample support with the vacuum lock chamber while the plurality of samples on another of the sample supports are being struck with laser pulses.
0. 71. The method as defined in
controlling an x-y table in response to the computer for positioning the plurality of samples within the sample receiving chamber of the mass spectrometer.
0. 72. The method as defined in
supporting each of the plurality of sample supports on an electrically conductive block within the sample receiving chamber; and
electrically insulating the x-y table from the electrically conductive block.
0. 73. The method as defined in
temporarily affixing the position of a respective sample support with respect to the electrically conductive block.
0. 74. The method as defined in
adjusting the intensity of a laser beam output from the laser source in response to the computer.
0. 76. The system of
0. 77. The system of
0. 78. The system of
0. 79. The system of
0. 80. The system of
0. 81. The system of
0. 82. The system of
0. 83. The system of
0. 84. The system of
0. 85. The system of
0. 86. The system of
0. 87. The system of
0. 89. The system of
0. 91. The method of
0. 92. The method of
recording in a computer mass data corresponding to at least one of the plurality of samples struck with a laser pulse.
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comers corners 22 yet provides a total square surface having 50 mm sides interior of the beveled comers corners on the top surface of the plate 10 for receiving multiple samples. Samples may be deposited on this plate in a variety of ways, and for explanation purposes it may be assumed that an array of circular spots 16 is photoetched into the plate 10 along with identifying numbers. This arrangement easily accommodates up to 1024 sample spots each 1 mm in diameter in a 32×32 array without identifying numbers. Each of these 1024 sample spots will accommodate about 100 nanoliters of sample solution.
As shown in
As shown in
2. Identification of Sample Position and Plate
The x-y coordinate of each sample position on one side (typically the top side) of the sample plate may be used to determine a unique sample position on each sample plate. The diameter of a sample spot centered on each position may be used to further define a sample position. The minimum data required to uniquely identify a sample position is the x-y coordinate and the diameter of the spot. As discussed above, the sample position may be further defined by a photoetched well or photoplated spot centered at the corresponding x-y coordinate on the sample plate, and may be even further defined by the corresponding number etched or plated near the corresponding sample spot.
Each particular sample plate may be identified by a serial number etched into the top surface of the plate or attached to or etched into the bottom surface of the plate. A computer readable bar code may be used with a sufficient number of digits to uniquely identify the sample plate relative to any other which might be encountered within a series of similar runs. The systems involved in applying the samples to the sample plates and those for loading the plates into the mass spectrometer as discussed below may also be equipped with bar code readers to provide the required identification of the sample plates.
3. Processing and Preparing Samples
The details of this component will depend on the application, the types of samples to be tested, and the degree to which the samples are prepared and purified prior to being input to the analysis system described below. The following discussion sets forth the representative steps required to carry out an automated MALDI analysis. It should be appreciated that additional automated sample preparation and purification steps could be added. Rate-determining steps may be used, for example, to determine the speed with which the complete determination can be done.
The invention is particularly suited for DNA sequencing. For this purpose, it is assumed that a set of sequencing mixtures has been prepared off-line using either the Maxxam-Gilbert or Sanger method. The mixtures may be presented to the system in the form of liquid solutions in small vials or tubes in a tray which may be accessed by an autosampler. Substantially the same samples in the same form may be presented for separation by electrophoresis in conventional DNA sequencing.
With reference to
4. Drying and Storing Sample Plates
When each sample location on a plate has been loaded with a sample, the samples are allowed to dry before the plate is transferred into the vacuum chamber of the mass spectrometer. In the simplest case, the plates may be transferred from the sample loading system to a rack or cassette where they are allowed to dry in laboratory air. In the preferred embodiment, however, this rack or cassette 54 is located inside a sealed chamber 52 equipped with a computer-controlled door 56 which allows the samples to be dried in an environment in which the pressure, temperature, and composition of the surrounding atmosphere is controlled. In the fully automated mode, each of the loaded and dried sample plates may be transferred from the sample plate storage chamber 52 to an adjacent mass spectrometer. Alternatively, the samples may be prepared and loaded off-line onto the sample plates. When a sufficient number of sample plates has been loaded with samples, the plurality of sample plates may be transferred manually to the mass spectrometer and loaded as a complete cassette using the manually operated sample loading door.
5. Transferring Sample Plates into the Mass Spectrometer Sample Receiving Chamber
The manual step involved in loading the sample plates may be eliminated by adding a sample storage region to the vacuum lock chamber of a mass spectrometer, as shown schematically in
The system as shown in
When analysis of the samples on one plate 10 within the ion source is completed, the plate 10 is ejected and placed in a vacant slot in the sample storage cassette 80. This cassette 80 is then moved by stepper motor 66 and lead screw 64 to bring a new sample plate in the transport tray 80 in line with the transporter 89, and the new sample plate is loaded. The exchange of samples may thus be accomplished without venting of the vacuum lock chamber 68, which was evacuated during the time that the samples on the previous plate were being analyzed. This allows sample plates to be changed very quickly (at most a few seconds) while maintaining the ion source at high vacuum.
The sample storage chamber 60 is equipped with a manually operated door 70 through which a number of sample plates loaded with samples that are off-line can be introduced simultaneously. To load a set of samples, a “manual load” setting is selected on the computer 36. This causes the sample storage chamber 60 to be vented to atmosphere via vent valve 72, and allows the manual load door 70 to be opened. The samples are then loaded and the chamber evacuated. The entire set of sample plates can now be analyzed automatically without further operator intervention.
6. Automated Vacuum Lock System
The vacuum lock chamber 68 is equipped with computer controlled valves and mechanical transport devices which allow the sample plates 10 to be transported under computer control from the sample storage chamber 60 (which may be at atmospheric pressure) to the sample receiving stage within the evacuated ion source chamber 74 of a mass spectrometer, without venting the evacuated chamber 74. The vacuum lock chamber 68 has an input port which may be opened or closed by door 58 and through which sample plates are loaded from the sample storage chamber 60 into the vacuum lock chamber 68. An output port through which a sample plate is transported from the vacuum lock chamber 68 to the ion source vacuum chamber 74 is similarly opened and closed by output door 76. Each door includes an “O” ring seal and may be opened and closed by a respective air cylinder 75 controlled from the computer 107.
A preferred embodiment of the vacuum lock chamber 68 is depicted in
A simplified version of the vacuum lock designed for use with remote sample storage chamber is shown schematically in
With reference now to
To eject the sample plate and load a new one the process is reversed. First the output door 76A is opened, and the transport cylinder 89A equipped with the electromagnet 102 is extended so that the electromagnet makes contact with the magnetic strip on the sample plate 10. The electromagnet is energized and the cylinder 89A retracted to move the sample plate from the ion source chamber 97 to the transport tray 99 in the vacuum lock chamber 92. The output door 76A is closed, the magnet 102 is de-energized, the input door 98 is opened, and the sample tray 99 extended so that the old sample plate can be removed by the operator and replaced with a new sample plate. Except for this final step, the entire operation is accomplished entirely under control of computer 107 with no intervention from the operator except for selecting a “eject” setting on the computer to remove a sample, and an “operate” setting to load a new sample and begin the test.
Operation of the fully automated system shown in
7. Sequentially Testing Loaded Sample Plates
A preferred embodiment of the ion source 110 and a MALDI mass spectrometer 112 is depicted in
With computer control of the stepper motors, this system allows any selected point on the sample plate to be positioned precisely (typically within one thousandths of an inch) on the optic axis of the mass spectrometer where it is irradiated by the laser beam 136. Beam 136 strikes a sample on plate 10 at point 120 within plane 117, resulting in ion beam 134. Accordingly ions may be produced from each sample on the plate 10, which is moved automatically by the x-y table 114 between sample positions with respect to the laser beam.
The remaining components of a suitable time-of-flight mass spectrometer 112 as shown in
Most of the low weight ions are prevented from reaching the detector 140 by deflection plates 130 and 132, which may be spaced 1 cm. apart. Plate 130 may be a ground potential. Plate 132 receives a square wave pulse timed as a function of the laser beam striking a particular sample. Each pulse thus suppresses low mass ions, so that substantially only desired ions reach the detector 140. Other details with respect to a suitable spectrometer are disclosed in U.S. Pat. Nos. 5,045,694 and 5,160,840.
8. Automatically Adjusting Laser Intensity and Sample Position
In MALDI, the intensity and quality of the mass spectra generated is strongly dependent on the intensity of the plume of ionized and neutral material that is produced by the incident laser pulse impinging on the sample and matrix. This intensity depends on the laser intensity, the composition of the matrix used, and details of the crystalline structure of the matrix and sample on the surface. While it is possible to establish a narrow range of laser intensities which produce acceptable spectra, one typically cannot predict with the desired precision the laser intensity which will yield the best results on a particular sample. In general, if the laser intensity if too high, the signal-to-noise ratio may be excellent, but the mass resolution and mass accuracy is degraded. Conversely, if the laser intensity is too low, the mass resolution and accuracy are satisfactory, but the signal level is low and signal-to-noise ratio is poor. Also, the surfaces of multiple samples on a plate tend to be non-uniform, so that some locations yield excellent results and others do not. Under manual control of the laser beam and sample position, it is possible through a process of trial and error to find a combination of laser intensity and sample position which provides excellent results.
An automatic control used according to this invention closely mirrors what is generally the most successful strategy when operating manually. The intensity of the beam output 136 from the laser source 148 is increased until the ion signal suddenly appears at a relatively high setting. At this point, signal-to-noise is excellent, but resolution is poor. As the laser intensity is decreased, the signal may actually increase at first (sometimes going into saturation), but at some lower intensity the signal is decreased, and the resolution is dramatically increased. With an improved attenuator 138, this hysteresis appears to be entirely related to changes in the sample properties, and is not due to hysteresis in the attenuator. The upper and lower values for these events are very reasonably reproducible and appear to depend primarily on the particular matrix used, and only weakly on the sample preparation, source voltage, or other parameters.
The strategy for exploiting these observations in the automatic mode follows. The upper and lower limits in the acquisition set-up menu and the laser step size are established. Two choices are provided for the number of spectra to be averaged: an upper number and a lower number. The upper number of spectra are averaged when the laser beam 136 is at its maximum intensity, and the lower number is used at all other laser intensities.
When a new sample is selected by the autosampler menu, the acquisition starts with the laser beam 136 set at the upper limit. The number of spectra requested is averaged. If a spectrum acquired contains intensity within the desired mass and intensity limits set, the spectrum is saved and calibrated using the upper calibration file associated with this set-up file. If the spectrum acquired is too intense, i.e., the maximum intensity within the mass window is greater than the upper intensity level (typically set just below saturation), the laser intensity is decreased by one increment and the process repeated until a spectrum meeting the selection criteria is obtained or the lower limit is reached. If the spectrum is too weak, i.e., the maximum intensity within the mass window is too weak, the sample is incremented to a new spot and the process is repeated. If a spectrum is obtained which has intensity within the chosen limits at any laser intensity other than the lower limit, that spectrum is saved as an upper intensity spectrum and the upper calibration file associated with the acquisition set-up file is used. If an acceptable spectrum is obtained at the lower limit of laser intensity, that spectrum is saved as a lower intensity spectrum and the lower calibration file associated with the acquisition set-up file is used. If both an upper and a lower intensity spectrum are obtained on the selected sample spot, the acquisition proceeds to the next sample. If only one of these is obtained, or neither one, the sample is incremented to a new spot until both an upper and a lower spectrum have been saved, or until the range of possible sample spots has been exhausted.
9. Automatically Calibrating the Mass Axis
During automatic operation of the MALDI instrument, an automatic procedure may be used for checking the calibration of and recalibrating the mass scale to maintain the desired mass accuracy. This can be accomplished by loading a sample plate containing one or more known samples so that the known mass spectrum can be used to automatically check and correct the mass scale as necessary.
The procedure for calibrating the mass axis is described below. Each acquisition set-up file must have both an upper and a lower calibration file associated with it. These files may be chosen from a list of files already in existence by the operator preparing the set-up file, or may be generated using the “calibrate” selection in the set-up file for calibration based on a selected known sample. Each calibration file which is saved may have all of the parameters associated with its generation saved, so that in the event the operator chooses a calibration file which employs different parameter values, a warning is given and the acquisition set-up file corresponding to the one that was used may be displayed with the parameters highlighted that are different from those which have been selected in the new acquisition set-up. The operator has the option of approving the chosen calibration file which is then associated with the new set-up file, even if some parameters are different. Alternatively, the operator may reject the chosen calibration file, return to the set-up file, and either choose a different calibration file or generate a new one. If a new calibration file is generated using a particular set-up file, a “check replace” selection may be employed to determine if the file is to replace a pre-existing calibration file. A new designation for upper or lower calibration numbers is also an option.
In addition to the above changes in the manual calibration procedure, an automatic calibration mode may be used. Particular samples on the sample plate may be identified as calibration samples, and the calibration compound selected from a list. For each sample or calibration compound, the matrix from a list may be selected. For each calibration compound and matrix combination chosen, a list of masses and laser intensities may be stored. The normally used mass and intensity valves values may be entered as an initial equipment set-up. A service technician will be able to alter initial factory data at the location of the customer.
During automatic calibration, the procedure for acquiring the calibration spectrum is the same as for acquiring data from a sample. If the calibration designation is selected in the autosampler set-up, that sample is treated as a calibration sample and the spectrum obtained is compared to that expected from the reference file. If peaks are found within the default values of mass and internally (typically set by the service technician), the calibration file for the particular acquisition set-up and laser intensity being used is recomputed, and the old file replaced by the new file. If the observed spectrum falls outside the default limits, a warning message is momentarily displayed and then stored for later display when the data are processed. If the attempted calibration does not succeed, the old value is retained, and automatic acquisition proceeds. For instrument service purposes, it may be desirable to retain the old calibration files in a directory accessible to the service technician.
To implement the above, columns may be added to the autosampler set-up menu. These columns might include a choice of sample or calibrant, a choice of matrices from a pull-down list, and a pull-down menu showing the list of known calibrants. The operator may also enter new parameters characterizing a new calibrant within another column. The operator may also have the option of designating a matrix choice in the acquisition set-up file.
10. Automatically Interpreting the MALDI Mass Spectra
Mass spectra interpretation depend on the type of samples analyzed and the information required. The first step is to convert the observed time-of-flight spectrum into a mass spectrum, i.e., a table of masses and intensities for all of the peaks observed in the time-of-flight spectra. Peaks that are known to be due to the matrix or other extraneous material will normally be deleted from this list. This mass spectrum is obtained by calculating the centroid and integral intensity of each peak. The peak width may also be included (e.g., full width at half maximum) to provide a measure of the maximum uncertainty in the mass determination.
In the application to DNA sequencing, each set of four samples consists of one sample ending, so that all possible fragments ending in a specific base are included in each sample set. Accordingly, for each DNA fragment to be sequenced, there is a sample with all possible fragments terminating in C, T, A, and G, respectively. Each of these fragments is observed as a peak in the time-of-flight spectrum of that sample. By superimposing the four spectra, the sequence of bases can be read directly. Furthermore, the mass difference between any pair of peaks in these four spectra mass correspond to the total mass associated with the nucleotides in that portion of the sequence. This provides a significant redundancy in the results, which may be useful for analysis other than that involving the simple ordering of the peaks, a feature which is not available in electrophoresis. If a peak is very weak and is missed, or if two peaks are insufficiently resolved, a base may be missed by simple ordering. The mass difference observed between the next pair of adjacent peaks will thus show the error and allow correction. The computer may thus interpret the spectra and directly produce the sequence of bases in the DNA fragment. If there are any regions of the spectrum where the results may be consider considered ambiguous or unreliable, e.g., because the observed mass differences are inconsistent, those regions may be flagged so that the operator may perform either manual study or further automated analysis on those regions.
According to the technique of this invention a MALDI mass spectrometer is used rather than electrophoresis separation for DNA sequencing. Until recently, the MALDI technique was limited to single-stranded DNA fragments up to about 50 bases in length, but the range has now been extended to fragments as large as 500 bases in length.
Conventional large-scale sequencing is currently being done at a rate approaching 1 Mb per year of finished sequence. The cost of sequencing is in the vicinity of one U.S. dollar per base. A rate of 500 Mb per year is required for the Human Genome Project. A price of 20 cents per finished base is commensurate with the budget and goals of this project.
At the present stage of development, MALDI analysis of DNA fragments can be done readily on mixtures containing components less than 50 bases in length. Recent work suggests that this fragment length can be extended, perhaps as much as one order of magnitude to fragments 500 bases in length. Large scale sequencing would proceed much more rapidly by this technique if the fragments analyzed could be extended significantly. A reasonable goal is to be able to accurately analyze mixtures containing oligimers up to 300 bases in length. The resolution and sensitivity of presently available instruments is satisfactory. Even with the limitations imposed by the short segments, the MALDI technique with application of the present invention could be competitive with conventional approaches.
The present invention can readily handle at least 4 samples per minute, which corresponds with 50 base fragments to 50 bases of raw data per minute, since 4 separate samples are required to sequence each segment. A single instrument can run at least 1200 minutes per day to provide 60,000 bases per day of raw sequence. This is about 22 Mb/year from a single instrument. This is raw data, however, and the piercing together of fragments from short sequence generated data is likely to require considerable redundancy. Nevertheless, a single instrument, even with the limitations imposed by short segments, can surpass the total output of present conventional sequencing. The price for this instrument is about $200,000, and it should have a useful life of at least 5 years. Total cost for operating and maintaining the instrument (including amortization) should be less than $100,000/year. If the instrument produces 2 Mb of finished sequence/year, this corresponds to 5 cents/base. 250 such instruments would be required to provide sequences at the rate required by the Human Genome Project. If the length of the fragments analyzed can be extended, the speed will increase and the cost will rapidly decrease since less redundancy will be required. If the fragment length was increased to 300 bases, the raw data rate increases proportionally to about 120 Mb/year. The ratio of this raw rate to finished data rate should improve dramatically and may approach 50 Mb/year for a single instrument. In this case, ten instruments could provide the rate required by the Human Genome Project at a cost of 0.2 cent per base. Although this rate would not include the cost of sample preparation and data analysis, the rate and cost of raw sequence determination would no longer be the limiting feature.
It should be understood that this invention has been disclosed so that one skilled in the art may appreciate its feature and advantages, and that a detailed description of specific components and the spacing and size of the components is not necessary to obtain that understanding. Many of the individual components of the mass spectrometer are conventional in the industry, and accordingly are only schematically depicted. The foregoing disclosure and description of the invention are thus explanatory, and various details in the construction of the equipment are not included. Alternative embodiments and operating techniques will become apparent to those skilled in the art in view of this disclosure, and such modifications should be considered within the scope of the invention, which is defined by the following claims.
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