Atomic absorption spectroscopy

Abstract

A method and apparatus for carrying out atomic spectroscopy, and particularly atomic absorption and atomic fluorescence spectroscopy. The method involves passing the emission spectrum of a light source through an atomized sample, changing the relationship between a selected emission line of the emission spectrum and a corresponding absorption line of the atoms of interest and measuring the absorption of that emission line by the sample before and after the aforementioned change in relationship. The change in emission and absorption line relationship can be effected by application of the zeeman Effect, Stark Effect, or Doppler Effect. The apparatus, in one form, includes an electro-magnet operative to apply a magnetic field to the atomized sample and thereby cause splitting and shifting of the aforementioned absorption line, and the magnet is modulated to effect periodic variation of the spectral line relationship.

Description

This is a continuation of application Ser. No. 376,498 filed July 5, 1973, now abandoned, which is a continuation of application Ser. No. 208,772 filed Dec. 16, 1971, now abandoned.

This invention relates to a method and means for carrying out atomic spectroscopy such as used for the analytical determination of various elements, and is applicable to atomic absorption spectroscopy (AAS) atomic fluorescence spectroscopy (AFS) or any other form of spectroscopy where a source emitting discrete lines is used and there is absorption of the line radiation by a substance with a narrow absorption profile (a narrow absorption line width). As a matter of convenience however, the invention will be hereinafter particularly described in relation to AAS.

In AAS the concentration of a chemical element in a sample is determined by measuring the degree to which atoms of the element absorb light of a wave-length which a (K-K_B)C β(K-K_B)C

would be reduced to (K_B1 -K_B2)C β(K_B1 -K_B2)C

where K_B1 ≈K_B2 because B₁ ≈B₂

and hence (K_B1 -K_B2)C β(K_B1 -K_B2)C can be made small. Thus by sequencing the light intensity measurements so that instead of a maximum field--zero field sequence, we have a maximum field--near maximum field sequence, it is possible to measure higher concentrations than can be measured by conventional AA. In essence the absorption of the atoms is being measured when the atoms are most transparent to the detuned incident radiation.

It has been suggested that the modulating means--e.g., magnetic field--can be applied to the light source as shown in FIG. 2 rather than than to an atomized sample as particularly described in relation to FIGS. 1, 3, 4 and 8, and whilst that remains a valid possibility, it is presently thought that best results will be usually obtained by modulating the atoms of the sample. That is, considering employment of the Zeeman Effect for example, application of the magnetic field to the atomized sample results in an automatic correction for lamp drift. In addition, application of the magnetic field to the atomized sample avoids difficulties in calibration that will normally result from modulating the lamp. By way of explanation, application of the magnetic field to the lamp tends to introduce non-linearity into the calibration (i.e., the absorption versus concentration graph), whereas application of the magnetic field to the atomized sample provides for linear calibration which is much simpler to deal with.

In order for the atomic absorption to be linear in calibration it is necessary for the light source to emit atomic spectral lines of the element to be determined, that are narrow compared with the absorption line to be measured. Application of the magnetic field to the lamp would in effect cause broadening of the emission spectral lines thereby creating a less favourable condition, whereas application of the magnetic field to the atomized sample causes broadening of the absorption line so enhancing the desired relationship between the emission lines and the absorption line.

It will be understood from the foregoing that application of the magnetic field, or other modulating means to the atomized sample achieves the dual function of background correction and light source monitoring.

In practice, some magnetic modulation of the atomic emission will occur when the magnetic field is applied to the atomized sample, and in the embodiment of FIGS. 1, 3, 4 and 8 as previously described, electronic correction of that modulation can be effected by looking at the emission at or near zero and maximum field phases of the cycle.

Both the method and apparatus particularly described in this specification involve the use of a single light source, but it is possible to embody the invention in a method and apparatus involving the use of two separate light sources.

It will be clear from the foregoing description that the present invention provides an extremely simple and yet effective method and means for conducting atomic spectroscopy. In particular, the invention overcomes the inaccuracies in readout resulting from non-atomic absorption and lamp drift in conventional single beam atomic absorption.

Finally, it is to be understood that various alterations, modifications and/or additions may be introduced into the methods, and constructions and arrangements of parts previously described without departing from the spirit or ambit of the invention.

Claims

1. Atomic spectrum analysis apparatus for elements exhibiting an anomalous zeeman splitting characteristic including a light source made from an element exhibiting an anomalous zeeman splitting characteristic, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and transverse magnetic field means operative upon said atomized sample to cause anomalous zeeman splitting of the absorption profile of said cloud of atoms, means to cause said photoelectric detection means to sense the effect of said splitting in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, wherein said means to cause said photoelectric detection means to sense the effect of said splitting includes means to modulate said magnetic field.

2. Atomic spectrum analysis apparatus including a light source providing radiation derived from an element exhibiting an anomalous zeeman splitting characteristic, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and magnetic field means operative upon said atomized sample to cause anomalous zeeman splitting of the absorption profile of said cloud of atoms, means to cause said photoelectric detection means to sense the effect of said splitting in the relationship between said selected emission line and a corresponding anomalous absorption line of said atomized sample, wherein said means to cause said photoelectric detection means to sense the effect of said splitting includes means to alternately pass different portions of said transmitted beam to said detector.

3. The apparatus of claim 2 wherein said magnetic field means comprising an electromagnet having pole faces separated by an air gap between which faces, in operation, said cloud of atomized sample is disposed, said poles of said electromagnet being displaced from said atomizing means to provide an ingress and egress

for cooling gases to said pole faces. 4. Atomic spectrum analysis apparatus including, a light source, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, an magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light,

including control means wherein said light source and said magnetic field means are both actuated responsive to said control means which is operative to energize said light source when said magnetic field is de-energized, to de-energize said light source when said magnetic field is energized, and to re-energize said light source when said magnetic field

is substantially at maximum magnitude. 5. Apparatus according to claim 4, wherein said control means includes a switch device through which power is supplied to said magnetic field means, and a triggering circuit operatively connected to said switch device and responsive to phase changes in the supply of said power so as to effect a predetermined time delay between de-energization and re-energization of said magnetic field

means. 6. Atomic spectrum analysis apparatus including, a light source, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, wherein said magnetic field means includes an electromagnet having its two pole ends and associated coils disposed on opposite sides respectively of a region above said atomizing means wherein said cloud of the atomized sample will be formed, one said coil being arranged with its windings extending transverse to the respective end portion pole ends of the electromagnet, and the other said coil being arranged with a portion of its windings extending substantially parallel to the respective end

portion pole ends of the electromagnet. 7. Apparatus according to claim 6, wherein said atomizing means includes an elongated burner body located between the two pole end faces ends of said electromagnet so that each said pole end face overlaps a respective side face of said burner body, and a space is defined between each said side face of the burner body and the overlapping pole end face of the electromagnet so as to form an air passage, said air passage being arranged so that during operation of said burner a flow of air is induced over each said pole end face of the electromagnet so as to prevent direct contact of the burner flame with said end faces two pole ends and thereby guard against overheating of said

electromagnet. 8. Atomic spectrum analysis apparatus including, a light source, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detection and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, wherein said magnetic field means and said atomizing means are attached against relative movement and are rotatably mounted so as to enable alteration of the relationship between said cloud of the atomized sample

and said path of said beam from said light source. 9. Atomic spectrum analysis apparatus including, a light source, carbon element atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, wherein said magnetic field means comprising an electromagnet having pole faces separated by an air gap between which faces, in operation, said cloud of atomized sample is disposed, said poles of said electromagnet being displaced from said atomizing means to provide an ingress and egress for cooling gases to said pole faces, including first means to periodically change the intensity of light emitted from said light source, second means to cause said magnetic field means to periodically change the relationship between said selected emission line and a corresponding line of said atomized sample, control means for causing the frequency of each said first and second means to be

synchronously related. 10. The apparatus of claim 9 wherein said control means includes means for causing said light source to be on when the magnetic field is a first predetermined value and said light source to be switched off when the magnetic field exceeds a predetermined second value, and where said light source is switched on again when said magnetic field

value reaches a third predetermined value. 11. The apparatus of claim 10 wherein said first predetermined value is substantially zero, and said second third predetermined value is the maximum

magnetic field value. 12. The apparatus of claim 10 wherein said first predetermined value is greater than zero in order to increase the dynamic

range of concentration measurements. 13. Atomic spectrum analysis apparatus including, a light source, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light wherein said magnetic field means includes a first coil having a first axis and a second coil having a second axis, said first and second coil being disposed about a core of magnetic material having a pole face on each end of said core, said magnetic core extending between said first and second coil, said pole faces being substantially parallel and separated by an air gap, said second axis of said second coil and said first axis of said first coil forming a plane which is perpendicular to

said pole faces. 14. The apparatus of claim 13 wherein said first axis of said first coil is perpendicular to said pole faces and said second axis

of said second coil is parallel to said pole faces. 15. Atomic spectrum analysis apparatus including, a hollow cathode lamp light source, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, including control means wherein said light source and said magnetic field means are both actuated responsive to said control means which is operative to energize said light source when said magnetic field is de-energized, to de-energize said light source when said magnetic field is energized and to re-energize said light source when said magnetic field is

substantially at maximum magnitude. 16. Apparatus according to claim 15, wherein said control means includes a switch device through which power is supplied to said magnetic field means, and a triggering circuit operatively connected to said switch device and responsive to phase changes in the supply of said power so as to effect a predetermined time delay between de-energization and re-energization of said magnetic field

means. 17. Atomic spectrum analysis apparatus including, a hollow cathode lamp light source, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and magnetic field means operative upon said atomized sample, to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, wherein said magnetic field means includes an electromagnet having its two pole ends and associated coils disposed on opposite sides respectively of a region above said atomizing means wherein said cloud of the atomized sample will be formed, one said coil being arranged with its windings extending transverse to the respective end portion pole ends of the electromagnet, and the other said coil being arranged with its windings extending substantially parallel to the respective end portion pole ends of the

electromagnet. 18. Atomic spectrum analysis apparatus including a hollow cathode lamp light source, carbon element atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source,

photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample,

magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample,

means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, wherein said magnetic field means comprises an electromagnet having pole faces separated by an air gap between which pole faces, in operation, said cloud of atomized sample is disposed, said poles pole faces of said electromagnet being displaced from said atomizing means to provide an ingress and egress for cooling gases to said pole faces, first means to periodically change the intensity of light emitted from said light source, second means to cause said magnetic field means to periodically change the relationship between said selected emission line and a corresponding line of said atomized sample,

control means for causing the frequency of each said first and second means

to be synchronously related. 19. Atomic spectrum analysis apparatus including, a light source, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source,

photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample,

magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample,

means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, first means to periodically change the intensity of light emitted from said light source, second means to cause said magnetic field means to periodically change the relationship between said selected emission line and a corresponding line of said atomized sample, and

control means for causing the frequency of each said first and second means to be synchronously related.

20. Improved apparatus for atomic absorption spectroscopy of a selected element exhibiting an anomalous zeeman characteristic;

a radiation source for providing a probe beam, said radiation source comprising said selected element which exhibits an anomalous zeeman splitting characteristic;

an atomizer adapted to receive a sample to be analyzed for the concentration of said selected element in said sample, said atomizer providing in operation, a cloud of atoms including atoms of said sample and background absorbers, if any, into said probe beam;

magnet means for providing a magnetic field substantially transverse to said probe beam, said magnetic field being applied, in operation, to said atomized atoms for causing said atoms to split;

means for selecting a first portion of said probe beam radiation transmitted through said atomizer, which first portion is reduced in intensity due to absorption by said cloud of atoms and background absorbers;

means for selecting a second portion of said probe beam radiation transmitted through said atomizer, which said second portion is reduced in intensity due to absorption by said background absorbers only;

means for photoelectrically detecting and measuring the intensity of said selected first and second portions of said transmitted probe beam; and

means connected to said means for photoelectrically detecting and measuring said first and second selected portions of said transmitted beam for determining a measure of the concentration of atoms of said selected element in a sample introduced into said atomizer as a function of the intensity of said first and second portion of said transmitted beam.

21. Apparatus according to claim 20 wherein said means for selecting said first portion of said probe beam radiation includes a polarizer between said radiation source and said photoelectric detection means. PAR

22. Apparatus according to claim 21 wherein said polarizer also comprises the means for selecting the second portion of said probe beam and wherein said means for selecting said first portion and second portions of said probe beam radiation includes means for modulating said polarizer to pass said first portion of said probe beam radiation to said photoelectric detection means for a first period of time and to pass said second portion of said probe beam radiation to said photoelectric

detection means for a second period of time. 23. A method of atomic spectrum analysis of elements exhibiting an anomalous zeeman splitting characteristic including the steps of: dissociating a sample into its atomic elements; directing a beam of light from a light source made from an element exhibiting an anomalous zeeman splitting characteristic through said atomized sample, the wave lengths of the atomic emission spectrum of said light source including the absorption wave lengths of a particular element sought to be detected in said sample, selecting a spectral line of said emission spectrum that corresponds to an absorption line of said atomized sample and therefore has a wave length profile which overlaps the wave length profile of said absorption line; applying a periodic transverse magnetic field to said atomized sample thereby inducing a change in at least one of said wave length profiles so that the degree of overlap of said profiles alternates between a plurality of values; photoelectrically detecting the energy from said selected emission line transmitted by said sample at said plurality of values of overlap; and electrically comparing the energy transmitted at one of said values with the energy transmitted at the other said value; generating a signal derived from said comparison, and providing an indication of said generated signal.

24. A method of atomic spectrum analysis of elements exhibiting an anomalous zeeman splitting characteristic including the steps of: dissociating a sample into its atomic elements; directing a beam of light from a light source made from an element exhibiting an anomalous zeeman splitting characteristic through said atomized sample, the wave lengths of the atomic emission spectrum of said light source including the absorption wave lengths of a particular element sought to be detected in said sample; selecting a spectral line of said emission spectrum corresponding to an absorption line of said atomized sample and which has a wave length profile which overlaps the wave length profile of said absorption line; applying a transverse magnetic field to said atomized sample to cause lateral displacement of components of said absorption spectral line; passing that part of said emission spectrum of said light source which passes through said atomized sample through a polarizer to select transmitted perpendicularly polarized components of said light source line; measuring the intensity of said transmitted perpendicularly polarized components respectively; and comparing said intensities to provide a measure of concentration of atoms of said element corrected for

absorption of said emission spectrum by said sample. 25. Atomic spectrum analysis apparatus including, a light source emitting a resonance line of an element exhibiting an anomalous zeeman line splitting characteristic, atomizing means for directing a cloud of an atomized sample including said element exhibiting an anomalous zeeman characteristic into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, a magnetic field means operative upon said atomized sample to induce a change in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, means connected to said photoelectric detection means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, and a control means wherein said light source and said magnetic field means are both responsive to said control means which is operative to energize said light source when said magnetic field is deenergized and to energize said light source when said magnetic field is substantially at maximum magnitude.

26. Atomic absorption analysis apparatus including, a light source made from an element exhibiting an anomalous zeeman splitting characteristic, atomizing means for directing a cloud of sample atoms exhibiting said anomalous splitting characteristic into said beam of light emitted from said source, means for detecting and measuring the intensity of said beam after transmission through said cloud of atoms, and means for determining the concentration of atoms in said cloud of atoms as a function of absorption of said beam of light, magnetic field means operative upon said atomized sample to induce a change in relationship between a selected emission line profile of said light source and a corresponding line profile of said atomized sample atoms, and control means to cause said magnetic field means to modulate said magnetic field and to cause said means for determining the concentration to compare the absorption when the magnetic field is near zero to the absorption when the

magnetic field is at a non-zero value. 27. Apparatus for atomic absorption including:

a light source made from an element exhibiting an anomalous zeeman splitting characteristic for providing a probe beam;

atomizing means for directing a cloud of sample atoms exhibiting said anomalous zeeman splitting characteristic into a beam derived from said light source;

means for applying a magnetic field to said cloud of sample atoms to cause said atoms to exhibit their anomalous zeeman splitting characteristic;

means for selecting and detecting the transmitted intensity of a first and second portion of said beam which has passed through said cloud of atoms, said first portion being reduced by absorption due to background and said second portion being reduced by absorption due to both background absorption and said sample atoms absorption;

means for determining the concentration of said anomalous characteristic atoms in said cloud of atoms as a function of said first and second portion by obtaining a comparison between said first and second portion of

said beam. 28. The apparatus of claim 27 wherein said means for applying a magnetic field provides a magnetic field transverse to said probe beam.

The apparatus of claim 27, wherein said means for selecting and detecting the transmitted intensity of a first and second portion of said beam includes means to modulate the magnetic field, means to photoelectrically detect transmitted light and means to substantially block the Pi component of said probe beam from reaching said photoelectric detector means.

30. The apparatus of claim 27, wherein said means for selecting and detecting the transmitted intensity of a first and second portion of said beam includes photoelectric detector means and variable polarizer means for selectively passing the Pi polarized or the Sigma

polarized portion of said probe beam. 31. Atomic spectrum analysis apparatus for elements exhibiting an anomalous zeeman splitting characteristic including a light source made from an element exhibiting an anomalous zeeman splitting characteristic, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and transverse constant magnetic field means operative upon said atomized sample to cause anomalous zeeman splitting of the absorption profile of said cloud of atoms, means to cause said photoelectric detection means to sense the effect of said splitting in the relationship between said selected emission line and a corresponding absorption line of said atomized sample, wherein said means to cause said photoelectric detection means to sense the effect of said splitting includes variable polarization means. 32. The apparatus of claim 31 wherein said magnetic field means comprise an electromagnet having pole faces separated by an air gap between which faces, in operation, said cloud of atomized sample is disposed, said poles of said electromagnet being displaced from said atomizing means to provide an ingress and egress for cooling gases to said pole faces. 33. Atomic spectrum analysis apparatus including a light source providing radiation derived from an element exhibiting an anomalous zeeman splitting characteristic, atomizing means for directing a cloud of an atomized sample into the path of a beam of light emitted by said source, photoelectric detection means for detecting and measuring the intensity of a selected spectral line of the atomic emission spectrum of said light source after said line has passed through said atomized sample, and transverse constant magnetic field means operative upon said atomized sample to cause anomalous zeeman splitting of the absorption profile of said cloud of atoms, means to cause said photoelectric detection means to sense the effect of said splitting in the relationship between said selected emission line and a corresponding anomalous absorption line of said atomized sample, wherein said means to cause said photoelectric detection means to sense the effect of said splitting includes means to alternately pass different portions of said transmitted beam to said detector. 34. The apparatus of claim 33 wherein said magnetic field means comprises an electromagnet having pole faces separated by an air gap between which faces, in operation, said cloud of atomized sample is disposed, said poles of said electromagnet being displaced from said atomizing means to provide an ingress and egress for cooling gases to said pole faces. 35. Improved apparatus for atomic absorption spectroscopy of a selected element exhibiting an anomalous zeeman characteristic,

a radiation source for providing a probe beam, said radiation source comprising said selected element which exhibits an anomalous zeeman splitting characteristic,

an atomizer adapted to receive a sample to be analyzed for the concentration of said selected element in said sample, said atomizer providing, in operation, a cloud of atoms including atoms of said sample and background absorbers, if any, into said probe beam,

magnet means for providing a constant magnetic field substantially transverse to said probe beam, said magnetic field being applied, in operation, to said atomized atoms for causing said atom's spectral lines to split,

means for selecting a first portion of said probe beam radiation transmitted through said atomizer, which first portion is reduced in intensity due to absorption by said cloud of atoms and background absorbers, and for selecting a second portion of said probe beam radiation transmitted through said atomizer, which said second portion is reduced in intensity due to absorption by said background absorbers only, means for photoelectrically detecting and measuring the intensity of said selected first and second portions of said transmitted probe beam, and

means connected to said means for photoelectrically detecting and measuring said first and second selected portions of said transmitted beam for determining a measure of the concentration of atoms of said selected element in a sample introduced into said atomizer as a function of the intensity of said first and second portion of said transmitted beam.

36. Apparatus according to claimm 35 wherein said means for selecting said first portion of said probe beam radiation includes a polarizer between said radiation source and said photoelectric detection means. 37. Apparatus according to claim 36 wherein said polarizer also comprises the means for selecting the second portion of said probe beam and wherein said means for selecting said first portion and second portion of said probe beam radiation includes means for modulating said polarizer to pass said first portion of said probe beam radiation to said photoelectric detection means for a first period of time and to pass said second portion of said probe beam radiation to said photoelectric detection means for a second period of time.

8. A method of atomic spectrum analysis of elements exhibiting an anomalous zeeman splitting characteristic including the steps of dissociating a sample into its atomic elements, directing a beam of light from a light source made from an element exhibiting an anomalous zeeman splitting characteristic through said atomized sample, the wave lengths of the atomic emission spectrum of said light source including the absorption wave lengths of a particular element sought to be detected in said sample, selecting a spectral line of said emission spectrum corresponding to an absorption line of said atomized sample and which has a wave length profile which overlaps the wave length profile of said absorption line, applying a transverse constant magnetic field to said atomized sample to cause lateral displacement of components of said absorption spectral line, passing that part of said emission spectrum of said light source which passes through said atomized sample through a polarizer to select transmitted perpendicularly polarized components of said light source line, measuring the intensity of said transmitted perpendicularly polarized components respectively, and comparing said intensities to provide a measure of concentration of atoms of said element corrected for

absorption of said emission spectrum by said sample. 39. Apparatus for atomic absorption including

a light source made for an element exhibiting an anomalous zeeman splitting characteristic for providing a probe beam,

atomizing means for directing a cloud of sample atoms exhibiting said anomalous zeeman splitting characteristic into a beam derived from said light source,

means for applying a transverse constant magnetic field to said cloud of sample atoms to cause said atoms to exhibit their anomalous zeeman splitting characteristic,

means for selecting and detecting the transmitted intensity of a first and second portion of said beam which has passed through said cloud of atoms, said first portion being reduced by absorption due to background and said second portion being reduced by absorption due to both background absorption and said sample atoms absorption, and

means for determining the concentration of said anomalous characteristic atoms in said cloud of atoms as a function of said first and second portion by obtaining a comparison between said first and second portion of said beam. 40. The apparatus of claim 39 wherein said means for selecting and detecting the transmitted intensity of a first and second portion of said beam includes photoelectric detector means and variable polarizer means for selectively passing the Pi polarized or the Sigma polarized portion of said probe beam.