ARTIFICIAL GENE AND METHOD FOR MUTATING GENE

Abstract

An artificial gene has a .sup.15N abundance exceeding a natural abundance in bases of at least a portion of DNA. A method for mutating a gene includes a first step of producing a state in which .sup.15N is unevenly distributed into a prescribed DNA in a living cell; and a second step of irradiation with a proton beam at an energy at which the .sup.15N produces a resonant nuclear reaction.

Claims

1. An artificial gene, wherein an abundance of .sup.15N in bases in at least a portion of DNA exceeds the natural abundance.

2. The artificial gene, according to claim 1, comprising a .sup.15N-unlabeled primer sequence and .sup.15N-labeled deoxyribonucleotide.

3. An artificial gene, comprising: the artificial gene according to claim 1; and a vector bonded to the artificial gene.

4. The artificial gene, according to claim 1, having a plurality of biomolecule binding sites, wherein the gene sequence is mutated in at least a portion of the plurality of biomolecule binding sites.

5. The artificial gene, according to claim 4, wherein the biomolecule is a protein.

6. An artificial gene that is a .sup.15N-unlabeled artificial gene and has a plurality of biomolecule binding sites, wherein the gene sequence is mutated in at least a portion of the plurality of biomolecule binding sites, and a .sup.15N-labeled biomolecule can bind to any of the plurality of biomolecule binding sites.

7. The artificial gene, according to claim 6, wherein the .sup.15N-labeled biomolecule can bind to a site, where the gene sequence is not mutated, among the plurality of biomolecule binding sites.

8. The artificial gene according to claim 7, wherein the biomolecule is a protein.

9. A kit comprising: the artificial gene according to claim 6; and a .sup.15N-labeled biomolecule capable of binding to any of the plurality of biomolecule binding sites.

10. A method for mutating a gene comprising: labeling a DNA with .sup.15N; and irradiating the DNA with a proton beam having energy at which .sup.15N undergoes a resonant nuclear reaction.

11. The method according to claim 10, wherein the labeling of the DNA with .sup.15N comprises replacing N in the DNA with .sup.15N.

12. The method according to claim 10, wherein the labeling of the DNA with .sup.15N comprises labeling the vicinity of the DNA with .sup.15N.

13. The method according to claim 10, wherein the labeling of the DNA with .sup.15N comprises binding a .sup.15N-labeled biomolecule to the DNA.

14. The method according to claim 13, wherein the biomolecule is a protein.

15. The method, according to claim 10, wherein the DNA in a living cell is labeled with .sup.15N.

16. The method, according to claim 15, wherein .sup.15N is maintained at the natural abundance in non-DNA cellular components in the living cell, and the .sup.15N abundance in the DNA is larger than the natural abundance.

17. The method, according to claim 15, wherein the labeling of the DNA with .sup.15N in the living cell comprises introducing into the living cell a .sup.15N-labeled deoxyribonucleotide and an inhibitor of glutamine synthetase.

18. The method according to claim 15, wherein the labeling of the DNA with .sup.15N in the living cell comprises introducing into the living cell a .sup.15N-labeled deoxyribonucleotide and an inhibitor of ribonucleotide reductase.

19. The method, according to claim 17, wherein the labeling of the DNA with .sup.15N in the living cell further comprises introducing .sup.15N-unlabeled glutamine into the living cell.

20. The method, according to claim 10, further comprising detecting the resonant nuclear reaction.

21. The method, according to claim 20, wherein an amount of 4.43 MeV gamma-ray is counted in the detection.

22. The method, according to claim 21, further comprising calculation, based on the amount of gamma-ray counted, the number of mutations produced in the DNA.

23. The method according to claim 22, wherein the amount of gamma-ray produced by a resonant nuclear reaction that occurs in a reference sample in which the number of .sup.15N atoms is known is referred in the calculation.

24. The method, according to claim 10, further comprising changing energy that produces the resonant nuclear reaction of .sup.15N.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0028] FIG. 1 is a diagram that shows, with reference to a method for mutating a gene according to an embodiment of the present invention, a DNA molecule in which the N presents in each of the base pairs has been replaced with .sup.15N.

[0029] FIG. 2 is a diagram that shows a depiction of the occurrence of a resonant nuclear reaction in a DNA molecule.

[0030] FIG. 3 is a diagram that shows the case of the use of a method for mutating a gene by irradiation with a heavy ion beam, which is a conventional art.

[0031] FIG. 4 is a diagram that shows an artificial DNA reference sample constructed of 84 base pairs.

[0032] FIG. 5 is a diagram that shows the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction.

[0033] FIG. 6 is a schematic diagram of a method for determining the presence/absence of DNA cleavage.

[0034] FIG. 7 is a diagram that shows an outline of a method for identifying the extent of cleavage in one strand of DNA strands.

[0035] FIG. 8 is a diagram that illustrates the synthesis of nitrogenous organic compounds in the cell.

[0036] FIG. 9 is a diagram that explains a novel method for the .sup.15N-labeling of only the nucleic acids in a cell in the case of the administration of MSX and .sup.15N-unlabeled glutamine.

[0037] FIG. 10 is a diagram that explains a process of the .sup.15N-labeling of only DNA in nucleic acid synthesis pathways.

[0038] FIG. 11 is a diagram that explains a novel method for carrying out .sup.15N-labeling of only a target gene or the neighborhood thereof.

[0039] FIG. 12 is a diagram that shows the gene structure of the pUC4-KIXX cyclic plasmid.

[0040] FIG. 13 is a graph that shows the resonance curve for the .sup.15N(p, α.sub.1γ).sup.12C resonant nuclear reaction for a .sup.15N_pUC4-KIXX plasmid sample.

[0041] FIG. 14 is a graph that shows the relationship between gene damage and the amount of proton beam irradiation of a plasmid. The proton beam-irradiated plasmid was introduced into Escherichia coli, and the E. coli was cultured on a culture medium to which ampicillin had been added.

[0042] FIG. 15 is a graph that shows the relationship between gene damage and the amount of proton beam irradiation of a plasmid. The proton beam-irradiated plasmid was introduced into E. coli and the E. coli was cultured on a culture medium to which kanamycin had been added.

[0043] FIG. 16 is a graph that shows the relationship between gene damage and the amount of proton beam irradiation of a plasmid. The proton beam-irradiated plasmid was introduced into E. coli and the E. coli was cultured on a culture medium to which ampicillin and kanamycin had been added.

DESCRIPTION OF EMBODIMENTS

[0044] Embodiments of the present invention will be described with reference to the appended figures. A feature designated by the same reference sign in individual figures has the same or similar structure.

[0045] The element nitrogen N is present in living organisms widely distributed among cell components from proteins, e.g., enzymes, to DNA. In a method for mutating a gene according to the present embodiment, a state is produced in which the isotope .sup.15N, which is present in living organisms at a natural abundance of 0.364%, is concentrated in and unevenly distributed into a target gene and substantial mutation is produced in the target gene by irradiating the target gene with a proton beam at the energy at which the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction takes place by .sup.15N and .sup.1H.

[0046] In the double-stranded DNA that constitutes a gene, five nitrogen atoms are bonded in adenine (A) in the purine ring and as an amino group and two nitrogen atoms are bonded in thymine (T) in the pyrimidine ring, and seven nitrogen atoms are thus present in the adenine-thymine pair (AT pair) in double-stranded DNA. Similarly, five nitrogen atoms are bonded in guanine (G), and three are bonded in cytosine (C), and eight nitrogen atoms are thus present in the guanine-cytosine pair (GC pair) in double-stranded DNA.

[0047] FIG. 1 shows a DNA molecule that possesses .sup.15N substituted for N in each base pair. The DNA molecule labeled with .sup.15N by 275.5 times concentrating the isotope ratio at which .sup.15N is naturally present is shown. .sup.15N has a natural abundance of 0.364%.

[0048] FIG. 2 shows a depiction of the occurrence of the resonant nuclear reaction in a DNA molecule. The .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction is taken place by a proton and single .sup.15N nucleus in the .sup.15N labeled DNA. The .sup.15N is extinguished and .sup.4He nucleus and .sup.12C nucleus are emitted in an substantially isotropic direction but are just opposite to each other centered on the bonding position of the .sup.15N atom prior to the reaction. They immediately capture electrons and traverse through the material as ions. They induce high-density electronic excitation of atoms in the vicinity area along the ion trajectory.

[0049] The probability of undergoing electronic excitation declines in inverse proportion to the square of the distance from the reaction center and is thus smaller for atoms as the distance of their location from the reaction center becomes far. That is, when .sup.15N undergoes the resonant nuclear reaction, atoms in the vicinity of the bonding position of the .sup.15N atom are locally affected by electronic excitation at a high probability. Accordingly, local modification takes place in the vicinity of the .sup.15N atom in the DNA.

[0050] FIG. 3 shows the reference case that has been used conventionally for mutagenesis to gene with irradiation of a heavy ion beam. Since the heavy-ion beam, which is conventionally used for mutagenesis to the gene, is uniformly incident on at a constant density throughout the DNA from the outside of DNA, the probability at which the DNA-atoms in a space in the vicinity of a heavy-ion trajectory suffer electronic excitation, and then the DNA is mutated, is constant throughout the whole area of the DNA.

[0051] In contrast to the above-mentioned reference case, the method according to the present embodiment enables the DNA around the biding position of a .sup.15N atom to be focally mutated at a high probability by raising the isotopic ratio of .sup.15N in or in the vicinity of the target gene.

[0052] The technique in the present embodiment of raising the isotopic ratio of .sup.15N in a target gene or neighborhood thereof is an art that directly utilizes the .sup.15N, natural abundance of which is 0.364% and is also present in living organisms. In addition, the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction also takes place in collision of a proton beam with the target .sup.15N presented in DNA of the organisms living on the surface of the Earth, where proton beam, which is the most probable hadron component in the cosmic rays in the sea level, is randomly poured on. The application of the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction in the present embodiment reproduces the same radiation effects as naturally induced on biological cells.

[0053] That is, the series of technique in the present embodiment: raising the isotopic ratio of .sup.15N in a target gene or neighborhood thereof, and a rise thereby in the probability of mutation in the target gene when the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction is induced by proton beam irradiation to the .sup.15N-labeled living cells, are nothing more than accelerating the same processes as of life on the Earth, which has been exposed to nature and suffered mutation in its gene information—since its appearance on the Earth. The principle of the fundamental mechanism in the method of the present embodiment is not at all different from the conventional methods to generate mutant strains by exposure to radiation (UV, X-ray, gamma-ray, and heavy-ion). Accordingly, since the principle in the method to generate mutation of a gene according to the series of technique in the present embodiment is different in principle from the genetic-recombination technique, the present method, which is not covered by the regulation on the genetic-recombination technology, enables one to generate the substantial mutation in a target gene.

[0054] A .sup.15N-labeled DNA reference sample having a precisely specified the number of .sup.15N atoms must be developed in order to quantitate mutation produced by the proton beam irradiation in a DNA sample, in which the isotopic ratio of .sup.15N is raised in a target gene or in the vicinity of the target gene in a living cell.

[0055] The .sup.15N-labeled DNA reference sample supports the acquisition of calibration data between the .sup.15N concentration in a DNA and the yields of 4.43 MeV gamma-rays emitted by the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction. Acquisition of calibration data of the yields of 4.43 MeV gamma-ray makes it possible—by detecting the yields of 4.43 MeV gamma-ray emitted by the resonant nuclear reaction at the same time as proton beam irradiation to the .sup.15N-labeled living cell and comparing this with the calibration values of the yields—to quantitate the number of mutations generated in the DNA in a living cell.

[0056] In the method for mutating a gene according to the present embodiment, a reference sample was constructed by the artificial synthesis by a polymerase chain reaction of DNA composed of .sup.15N-labeled base pairs. The reference sample of the constructed artificial DNA is desirably composed of a base sequence important in molecular biology, biochemistry, or biofunctionality.

[0057] FIG. 4 is a diagram that shows an artificial DNA reference sample constructed of 84 base pairs. The artificial DNA reference sample is constructed, for example, using the following method. An OR_WT_F oligonucleotide is synthesized by a polymerase chain reaction from a .sup.15N-unlabeled, i.e., containing .sup.14N at the natural abundance of 99.636%, OR_primer_F primer having the sequence structure of TACGTTAAATC at the 5′-end, and from 73 .sup.15N-labeled, i.e., containing .sup.15N at an abundance of at least 98%, deoxyribonucleoside 5′-triphosphates (.sup.15N-labeled dNTPs). An OR_WT_R oligonucleotide is also synthesized by a polymerase chain reaction from a .sup.15N-unlabeled OR_primer_R primer having the sequence structure of TGCAACCATT at the 5′-end, and from 74 .sup.15N-labeled dNTPs. A .sup.15N-labeled double-stranded DNA oligonucleotide, i.e., .sup.15N-labeled OR_DNA, is formed by the formation of base pairs between OR_WT_F and OR_WT_R by hydrogen bonding. This is used as the reference sample.

[0058] The .sup.15N-labeled OR_DNA is constructed of a total of 84 DNA base pairs (84 bps) from the .sup.15N-unlabeled primers OR_primer_F/_R and .sup.15N-labeled dNMPs (deoxyribonucleotide 5′-monophosphates). Excluding the primer, the base sequence itemization for the 73 bps in OR_WT_F is .sup.15N-labeled dAMP: 19, .sup.15N-labeled dTMP: 22, .sup.15N-labeled dGMP: 17, and .sup.15N-labeled dCMP: 15. Excluding the primer, for the 74 bps in OR_WT_R this is .sup.15N-labeled dAMP: 23, .sup.15N-labeled dTMP: 20, .sup.15N-labeled dGMP: 16, and .sup.15N-labeled dCMP: 15. This is summarized in the following Table 1.

TABLE-US-00001 TABLE 1 OligoDNA Oligonucleotide Primer Oligonucleotide Primer OR_DNA OR_WT_F OR_primer_F OR_WT_R OR_primer_R 84 base pairs 73 bases 11 bases 74 bases 10 bases dAMP 49 19 4 23 3 dTMP 49 22 4 20 3 dGMP 35 17 1 16 1 dCMP 35 15 2 15 3 Number of 623 269 39 280 35 nitrogen atoms .sup.15N isotope count 538.29 263.62 0.14 274.4 0.13 Molecular weight (g/mol) 52,467.00 26,234.64 26,232.36 98% .sup.15N label purity Molecular weight (g/mol) 52,477.95 26,240.00 26,237.95 100% .sup.15N label purity

[0059] The total number of N (.sup.14N+.sup.15N) contained in the .sup.15N-labeled OR_DNA is 623. The degree of .sup.15N purity is 98%, and the isotopic ratio of .sup.15N to .sup.14N varies in accordance with this degree of purity. When the degree of .sup.15N purity is 98%, the number of .sup.15N in the .sup.15N-labeled OR_DNA is 538.29. At an ideal 100% degree of .sup.15N purity, the number of .sup.15N in the .sup.15N-labeled OR_DNA has a maximum of 549.27, whose value corresponds to 88.17% of the total number of nitrogen atoms (refer to Table 1). The molecular weight of the .sup.15N-labeled OR_DNA also depends on the degree of .sup.15N purity and is 52,467 g/mol and has a maximum of 52,477.95 g/mol.

[0060] FIG. 5 shows the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction. When nuclei collide at 0.8409 MeV of a proton beam in the center-of-mass system (0.987 MeV in the laboratory system) accords with an energy difference between the nucleic binding energy of 12.1277 MeV in the .sup.15N and proton system and an excitation energy level of 12.9686 MeV in the .sup.16O* compound nucleus, the nuclear reaction occurs resonantly to produce .sup.16O* compound atomic nucleus. The .sup.16O* in the 12.9686 MeV level immediately brings about three kinds of reaction channels: the first reaction channel in which deexcitation to the 11.6007 MeV first excitation level of .sup.12C* occurs with the emission of an a particle; the second reaction channel in which deexcitation to the 7.1616 MeV ground state of .sup.12C occurs with the emission of an α particle; and a third reaction channel in which deexcitation to the 0 MeV ground state of .sup.16O occurs with the emission of only a gamma-ray. These are respectively represented by the nuclear reaction formulae (p, α.sub.1γ), (p, α.sub.0), and (p, γ.sub.0).

[0061] The (p, α.sub.1γ) reaction channel used in the present embodiment has the following characteristic features: an α (.sup.4He atomic nucleus), which has a higher ionization effects than the proton beam, and .sup.12C are emitted as secondary reaction particles; and a 4.43 MeV gamma-ray is emitted in every reaction by the deexcitation from the first excitation level of .sup.12C* to the ground state. Gamma-ray emission does not occur in the (p, α.sub.0) reaction channel, and emission of a secondary reaction particles having a high ionization effects does not occur in the (p, γ.sub.0) reaction channel. When .sup.15N is present within DNA or in the vicinity thereof, the emission of highly ionizing reaction secondary particles exercises a locally high ionization effects on the biomolecules in the vicinity of the .sup.15N and achieves the effect of providing a high probability of the generation of a desired gene mutation in the DNA. In addition, the 4.43 MeV gamma-ray emitted in every nuclear reaction can be easily detected, and this gamma-ray reflects the amount of gene mutation in the DNA that is produced by the irradiation with the proton beam. As a consequence, The detection of the 4.43 MeV gamma-rays when beam irradiation is performed achieves the effect of enabling quantitation of the amount of gene mutation in the DNA.

[0062] The resonance energy with the .sup.16O* second excitation level is much lower than the Coulomb barrier potential in the nuclear collision of the two atoms. Due to this, when the nuclear collision energy of the two atoms deviates from the resonance energy, exceeding the 300 eV resonance energy width defined as the width of the second excitation level of the .sup.16O* compound atomic nucleus, the reaction cross-section sharply decreases. That is, the proton beam incident at the resonance energy on the .sup.15N-labeled OR DNA causes the generation of the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction only within the range in which fluctuations in the incident energy fall within the resonance energy width.

[0063] In actual proton beam irradiation, the resonance energy width is determined by a convolution integration operation between the resonance energy width and the energy distribution of the proton beam, typically about 1 keV, and the proton beam irradiation energy is determined by adding the energy loss during the passage of protons through the substance to the resonance energy. That is, in the proton beam irradiation of a biological sample such as a .sup.15N-labeled DNA sample or a living cell containing .sup.15N_DNA, the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction can be produced everywhere in the .sup.15N distributed in a target sample from the surface into the interior, by causing the proton beam energy to change from the resonance energy to high energy exceeding the resonance energy, for example, by causing a change at a prescribed energy step width. The energy change width and the step width may be selected in correspondence to the target sample, and the resonance curve of the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction may then be acquired and determined. Refer, for example, to FIG. 13.

[0064] The α and .sup.12C* produced by the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction are emitted in opposite directions from each other, and when emission occurs in the same direction as the incident direction of the proton beam, the kinetic energy assumes a maximum value E(max) and becomes E.sub.C(max)=0.6252 MeV and E.sub.He(max)=1.2806 MeV for .sup.12C* and α, respectively. In addition, when .sup.12C* and a are emitted in the opposite direction from the incident direction of the proton beam, the kinetic energy assumes a minimum value E(min) and becomes E.sub.C(min)=0.1437 MeV and E.sub.He(min)=0.7991 MeV. .sup.12C* and α capture electrons immediately after emission to become .sup.12C and .sup.4He ions and proceed through the substance.

[0065] The .sup.12C and .sup.4He ions, constantly having values in these energy ranges, pass through the .sup.15N-labeled OR_DNA sample. Neighboring atoms along their ion trajectory, particularly neighboring atoms with a radius from at least 5 nm to not more than 10 nm, suffer electronic excitation. Even when proton beam irradiation is carried out at higher energy than the resonance energy—considering in advance that the target sample is not the .sup.15N-labeled OR_DNA sample, but a biological sample having a cell wall or organelles, e.g., eukaryotic unicellular algae, and energy loss occur when the protons pass through, e.g., the cell wall or organelles—a characteristic feature of the present method is that the reaction-generated .sup.12C and .sup.4He ions are emitted at certain energies, regardless of the irradiation energy of the proton beam, in the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction between the proton beam and .sup.15N-labeled DNA or a DNA-adjacent .sup.15N-labeled sample, and neighboring atoms along their ion trajectory suffer excitation at a certain intensity.

[0066] In addition, the electronic excitation from the reaction-generated .sup.12C and .sup.4He ions is given by the linear energy transfer (LET (MeVcm.sup.2/g)) and varies over the energy range in which the reaction-generated .sup.12C and .sup.4He ions are emitted. The LET to carbon C, which is one of the constituent elements of the target sample, is at least 2.51×10.sup.3 MeVcm.sup.2/g and a maximum of 4.70×10.sup.3 MeVcm.sup.2/g for the reaction-generated .sup.12C ion and is at least 1.73×10.sup.3 MeVcm.sup.2/g and a maximum of 1.99×10.sup.3 MeVcm.sup.2/g for the reaction-generated .sup.4He ion. These values are at least 17.2-times and a maximum of 27.1-times higher than the LET when protons traverse the .sup.15N-labeled OR_DNA sample at the resonance energy. Accordingly, a characteristic feature of the present method is that, for biological samples and particularly the .sup.15N-labeled OR_DNA sample, electronic excitation by the ions produced by the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction is very significantly higher than electronic excitation by proton beam irradiation, and the selective introduction of substantial mutation is thus made possible by the .sup.15N-labeling of a target gene.

[0067] The LET values for the reaction-generated .sup.12C and .sup.4He ions are at least 4.3-times and a maximum of 8.1-times higher than for typical heavy ion irradiation (for example, the 0.58×10.sup.3 MeVcm.sup.2/g, which is the LET to C in irradiation with the 320 MeV C ion). Furthermore, because the reaction-generated .sup.12C and .sup.4He ions are emitted from the DNA interior or from the vicinity of the DNA, the mutation is produced—in the .sup.15N-labeled OR_DNA sample or a living cell labeled with .sup.15N in the DNA or in the vicinity of the DNA—at a high probability in a gene near .sup.15N by a single .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction. The present method, therefore, enables the direction quantitation of the number of gene mutations produced in the vicinity of .sup.15N by counting the 4.43 MeV gamma-rays emitted from the first excitation level of the .sup.12C reaction product nucleus.

[0068] The mutation produced in the .sup.15N-labeled OR_DNA sample by proton beam irradiation is different from a biological sample having a DNA repair function, and DNA repair is not carried out. Accordingly, the pure physical mutation status induced by proton beam irradiation is clarified by analyzing the mutation of the .sup.15N-labeled OR_DNA sample. One method for analyzing the mutation produced in the .sup.15N-labeled OR_DNA sample is to determine the presence/absence of DNA cleavage by utilizing a cyclic plasmid vector or DNA having a cyclic shape that is present in the cytoplasm of, e.g., bacteria.

[0069] FIG. 6 shows an artificial gene provided by the ligation of the artificial gene shown in FIG. 4 into a different artificial gene and also shows an outline of a method for determining the presence/absence of DNA cleavage. A cyclized plasmid vector is produced by ligating the .sup.15N-labeled OR_DNA into an artificially synthesized linear plasmid (T-vector pMD19, 2,692 base pairs) that incorporates an E. coli gene that provides resistance to ampicillin, a β-lactam-type antibiotic used to treat infections, and this cyclized plasmid vector is introduced into a culture medium of E. coli. The cyclized plasmid vector is taken up by the E. coli, and the ampicillin-resistant E. coli propagate. When the .sup.15N-labeled OR_DNA has been preliminarily cleaved by proton beam irradiation, the plasmid vector does not become cyclic and is degraded in the E. coli cell and does not become a stable gene and the E. coli is then not resistant to ampicillin and dies. For the cyclic plasmid vector in which the .sup.15N-labeled OR_DNA is ligated, E. coli growth is slower as more cleaved .sup.15N-labeled OR_DNA is contained. Each of the following samples was ligated into T-vector pMD19: .sup.15N-labeled OR_DNA sample, .sup.15N-unlabeled OR_DNA sample, and .sup.15N-labeled OR_DNA for non-proton-beam-irradiation; and each was introduced into the ampicillin-containing culture medium, and the number of E. coli colonies was compared. With the .sup.15N-labeled OR_DNA sample, DNA mutation is produced by the proton beam and the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction. With the .sup.15N-unlabeled OR_DNA sample, DNA mutation is produced by only the proton beam. DNA mutation is not produced with the non-proton-beam-irradiated sample. This evaluation method clarifies the relative frequency of introduction of DNA mutation by the proton beam irradiation of the .sup.15N-labeled OR DNA.

[0070] The following is a method for more directly analyzing the status of cleavage of the .sup.15N-labeled OR_DNA by proton beam irradiation: introducing a phosphate group containing the .sup.32P radioisotope and separating the fragments by electrophoresis at a resolution of 1 base. This method enables the identification of the extent of cleavage in one of the DNA strands.

[0071] FIG. 7 shows an outline of a method for identifying the extent of cleavage in one strand of DNA strands. One of the primers, OR_primer_F or OR_primer_R, is first phosphorylated with ATP prior to PCR sample synthesis of the .sup.15N-labeled OR_DNA and during PCR sample synthesis, a DNA fragment is synthesized that has the phosphate group attached only to the 5′-end of one DNA chain. After proton beam irradiation, only the DNA chain to which the phosphate group is not attached is labeled with .sup.32P using [γ?.sup.32P]-ATP. When high-voltage electrophoresis at a low salt concentration on a urea-containing thin gel is used to separate the DNA in a single-stranded state (denatured state) while heating, the DNA can be distinguished at a single base difference. Since a single base difference can be distinguished by gel electrophoresis, it is possible to distinguish whether cleavage could be random or is prone to occur only in the vicinity of certain specific bases.

[0072] When the DNA within a living cell is labeled with .sup.15N, only the DNA is .sup.15N-labeled by discriminating between the nitrogen that constitutes the DNA and non-DNA nitrogenous intracellular molecules that constitute the living cell, for example, the nitrogen atoms present in protein, e.g., proteins that form the cell and enzymes that regulate metabolic functions, or the nitrogen present in the RNAs that carry out various functions in the cell, e.g., the ribosomal RNA that forms the ribosomes, the transfer RNA that transports amino acids, and the messenger RNA that specifies amino acid sequences at the ribosome.

[0073] The nitrogen in a cell is utilized in diverse nitrogenous organic compounds, e.g., amino acids, nucleotides, proteins, nucleic acids (DNA, RNA), and some lipids. For all of these nitrogenous organic compounds, an initial organic nitrogenous compound is produced by the glutamine synthetase-mediated reaction with glutamic acid of inorganic nitrogen in the form of the ammonium ion NH.sub.4.sup.+ to fix the same in an organic compound as glutamine (ammonia assimilation). An amino group is transferred from glutamine to 2-oxoglutaric acid by glutamate synthase to produce two molecules of glutamic acid. Numerous nitrogenous organic compounds are synthesized by the direct modification of the thusly produced glutamine and glutamic acid or by amino group transfer reactions.

[0074] FIG. 8 shows synthesis pathways for nitrogenous organic compounds in the cell. Nitrogenous compounds are degraded in the cell back to ammonia for recycling. Amino acids are used in the synthesis of structural proteins, enzymes, nucleic acids, and lipids for various uses. On the other hand, in the case of DNA, DNA synthesis proceeds from deoxyribonucleotides by the successive transfer of genetic information. When an artificially synthesized .sup.15N-labeled deoxyribonucleotide is introduced into the culture medium, it is taken up by the cell, and a portion is degraded, and the ammonium ion is synthesized, and protein synthesis is begun. In order to carry out the .sup.15N-labeling of only DNA, methionine sulfoximine (MSX), which is an inhibitor of glutamine synthetase, is introduced to inhibit this process so .sup.15N-labeled protein is not synthesized.

[0075] FIG. 9 shows a novel method for the .sup.15N-labeling of only the nucleic acids in a cell in the case of the administration of MSX and .sup.15N-unlabeled glutamine. Glutamic acid and ammonia for the amino group bind to the active site of glutamine synthetase to synthesize glutamine, and the glutamine is released from the glutamine synthetase. However, the structural formula for MSX contains the HN═S═O structure, and this resembles the H.sub.2N—CH═O in the structural formula for glutamine. In addition, as MSX has a strong active site, if glutamic acid and ammonia bind to it, they cannot be released from it and formation of glutamine is inhibited. That is, the cycle of glutamic acid synthesis by glutamate synthase from glutamine is interrupted, and .sup.15N-labeled protein is then not synthesized. However, .sup.15N-unlabeled glutamine is added to the culture medium so as not to interrupt the synthesis of proteins, which are required for numerous purposes. This results in the synthesis of structural proteins, enzymes, and some DNA.Math.RNA in which the .sup.14N abundance is 99.637%. Of the .sup.15N-labeled deoxyribonucleotide taken up into the cell, the remaining .sup.15N-labeled deoxyribonucleotide not committed to ammonia synthesis is used to synthesize DNA, and as a consequence, the performance of .sup.15N-labeling in the cell is limited to only DNA.

[0076] The process of the .sup.15N-labeling of only DNA in the nucleic acid synthesis pathways in the cell is shown in further detail in FIG. 10. In order to synthesize .sup.15N-labeled DNA, (1) cell culture is first carried out with .sup.15N-labeled deoxynucleotides for each of the four bases having been added to the culture medium. Then, since deoxyribonucleotides for DNA synthesis are synthesized only from ribonucleotides by ribonucleotide reductase (RNR), (2) an inhibitor of RNR (i-RNR) is introduced, and conditions are formed in which there is no synthesis in the cell of deoxyribonucleotides not labeled with .sup.15N. In addition, within the cell, (3) base transition occurs between deoxyribonucleotides and ribonucleotides, and the .sup.15N-labeled deoxyribonucleotide bases are introduced from outside the cell transition to ribonucleotide bases within the cell, and .sup.15N RNA can be directly synthesized. Conversely, the .sup.15N-unlabeled ribonucleotide bases also transition to deoxyribonucleotide bases. However, (4) the amount of .sup.14N_ribonucleotide metabolized from, e.g., .sup.14N_amino acids, in the cell reaches high levels due to the inhibition of RNR according to (2), and the amount of base transition from .sup.15N_deoxyribonucleotide to ribonucleotide can be inhibited. When, in (1), .sup.15N_deoxyribonucleotide is introduced into the culture medium in excess, exceeding the amount required for .sup.15N_DNA synthesis, this can create the likelihood in (3) that .sup.15N_base transitions from deoxyribonucleotide to ribonucleotide. Accordingly, the amount of .sup.15N_deoxyribonucleotide introduction into the culture medium can be adjusted as appropriate so as to provide a high .sup.15N_DNA synthesis efficiency and restrain .sup.15N_RNA synthesis.

[0077] FIG. 11 shows a novel method for carrying out .sup.15N-labeling of only a target gene or the neighborhood thereof. The base sequence of the .sup.15N-labeled OR_DNA shown in FIG. 4 is a portion of a gene from the lambda (λ) phage virus, which infects an E. coli host, and is a regulatory gene for suppressing its own growth in order for the λ phage to infect the E. coli host without killing the host. The .sup.15N-labeled OR_DNA has three Cro protein binding sites, and the regulatory gene is activated when the Cro protein binds to any one of the sites. The frequency of regulatory gene activation is regulated when, among the three binding sites, a location is introduced where the gene sequence has been mutated. FIG. 4 describes a method for producing .sup.15N-labeled OR_DNA by a polymerase chain reaction technique. In contrast to this, by synthesizing the 84-base pair OR_DNA without .sup.15N-labeling and then introducing this into the culture medium, when .sup.15N-labeled Cro protein is introduced to the E. coli that has taken up the regulatory gene, the .sup.15N-labeled Cro protein binds to the regulatory gene in the E. coli. When proton beam irradiation is carried out in this state, the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction occurs in the vicinity of the prescribed gene where the .sup.15N-labeled Cro protein is bound. This method enables mutation to be induced in a prescribed gene at high probabilities.

EXAMPLE 1

Results of Proton Beam Irradiation of a .SUP.15.N-Labeled OR_DNA Sample

(1) Preparation of .SUP.15.N-Labeled OR_DNA Sample

[Phosphorylation of OR_primer_R]

[0078] The phosphorylation process in support of the evaluation of DNA cleavage after proton beam irradiation is described as follows. ATP (10 mM=mmol/L): 16 μL, OR_primer_R (100 μM): 10 μL, 10×-diluted buffer solution: 16 μL, T4PNK: 8 μL, and sterile water: 110 μL were reacted for 35 minutes at 37° C.; the reaction was then stopped by heating to 72° C., and protein and lipids were removed by PCI extraction (phenol:chloroform:isoamyl alcohol (25:24:1) extraction); and this was followed by ethanol fixation and extraction.

[0079] [Synthesis of .sup.15N-Labeled OR_DNA by PCR Method]

[0080] Two types, with and without phosphorylated primer, were synthesized. 35 PCR cycles (98° C.-10 minutes, 31° C.-20 minutes, 72° C.-30 minutes) and finishing were carried out with each of: heat-resistant DNA polymerase (PrimeSTAR): 0.5 μL, 5×-diluted buffer solution: 10 μL, .sup.15N-labeled (.sup.15N purity≥98%) dNTP: 6 μL, OR_primer_F (10 μM): 2.5 μL, OR_primer_RP (phosphorylated primer 10 μM): 7.5 μL, template: 1 μL, sterile water: 22.5 μL, heat-resistant DNA polymerase (PrimeSTAR): 0.5 μL, 5×-diluted buffer solution: 10 μL, .sup.15N-labeled (.sup.15N purity≥98%) dNTP: 6 μL, OR_primer_F (10 μM): 2.5 μL, OR_primer_R (unphosphorylated primer 10 μM): 2.5 μL, template: 1 μL, sterile water: 27.5 μL. The synthesis of an 84 base pair DNA was confirmed by electrophoresis.

[0081] (2) Proton Beam Irradiation

[0082] Irradiation samples were prepared by dripping the .sup.15N-labeled OR_DNA sample or .sup.15N-unlabeled OR_DNA sample on an Au substrate. The OR_DNA solution concentration was 31.2 ng/μL, and the dripped sample provided by dripping an amount of 13 μL over a dripping area of 0.23 cm.sup.2 contained 4.7×10.sup.12 DNA with at least 538 .sup.15N atoms being bonded in each DNA. It was 1.1×10.sup.16 cm.sup.−2 converted to per the sample area. Proton beam irradiation was carried out using the 4 MV Pelletron electrostatic accelerator at the National Institute of Advanced Industrial Science and Technology, Tsukuba Center, and the 1 MV tandem electrostatic accelerator at the Research Facility Center for Science and Technology of Tsukuba University. The beam current was 0.1 nA to 5 nA, and the beam irradiation area was 0.071 cm.sup.2. The 4.43 MeV gamma-rays emitted by the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction were detected by placing, outside the vacuum at a distance of 24 mm from the irradiation sample, a EGO detector (Bi.sub.4Ge.sub.3O.sub.12 crystal scintillator, specific gravity 7.3 gcm.sup.−3, diameter 76.2 mm×length 79.2 mm), which contains .sup.83Bi and has the highest detection efficiency for high-energy gamma-rays. The detectable solid angle of the detector is 10% of the omnidirectional angle. When the detection sensitivity for 4.43 MeV gamma-rays is a maximum of 0.1, the detection efficiency for 4.43 MeV gamma-rays is a maximum of about 1%. When the .sup.15N-labeled OR_DNA sample was irradiated with a proton beam at constant energy, the 4.43 MeV gamma-ray count was 4,000 counts, and the total count for irradiation at 8 points over the energy of 8 keV was 25,000 counts. Considering the detection efficiency, mutation by the .sup.15N resonant nuclear reaction was produced in at least 2.5×10.sup.6 15N-labeled OR_DNA.

[0083] (3) Ligation of .sup.15N-Labeled OR_DNA into Linear Plasmid Vector:

[Preparation of A Protruding Ends in .SUP.15.N-Labeled OR_DNA]

[0084] Four types of mixed solutions were prepared and reacted for 1 hour at 72° C.: proton beam-irradiated .sup.15N-labeled OR_DNA (9 ng/μL): 6.9 μL, buffer solution (Ex taq) 1 μL, Ex taq 0.1 μL, dATP (10 mM) 2 μL, OR_DNA unirradiated sample (8 ng/μL): 6.9 μL, 10×-diluted buffer solution (Ex taq) 1 μL, Ex taq 0.1 μL, dATP (10 mM) 2 μL, negative insert DNA sample: 6.9 μL, 10×-diluted buffer solution (Ex_taq) 1 μL, Ex_taq 0.1 μL, dATP (10 mM) 2 μL, control insert CI sample (10 ng/μL): 6.9 μL, 10×-diluted buffer solution (Ex_taq) 1 μL, Ex_taq 0.1 μL, dATP (10 mM) 2 μL.

[0085] [Ligation with Linear Plasmid Vector]

[0086] The aforementioned four types of mixed solutions were mixed with a linear plasmid vector (T-Vector pMD19, 2,692 base pairs) on ice and, after standing for 30 minutes, a 30-second thermal shock at 42° C. was applied to increase the transformation efficiency.

[0087] [Culture of Ampicillin-Resistant E. Coli]

[0088] E. coli (JM109) that had been shaking-cultured on M9 culture medium at 180 rpm and a temperature of 37° C. was seeded to ampicillin-containing culture media into which the four types of cyclic plasmid vectors had been introduced, and colony formation by the JM109 was compared. 46 colonies/11 ng DNA was obtained for the culture medium that contained the cyclic plasmid vector ligated with the non-beam-irradiated sample, while a reduction to less one-third, or 13 colonies/11 ng DNA, was obtained for the culture medium that contained the cyclic plasmid vector ligated with beam-irradiated .sup.15N-labeled OR_DNA.

EXAMPLE 2

Results of Proton Beam Irradiation of E. Coli Biological Samples

[0089] Since proton beam irradiation is carried out substantially in a vacuum, the E. coli (JM109) was first converted into a freeze-dried state, and its durability was investigated. 10 μL of E. coli JM109 solution was introduced into an Eppendorf tube and was divided into a sample temporarily frozen at the temperature of liquid nitrogen and a sample not frozen by liquid nitrogen. Each was introduced into a vacuum dryer at −20° C. and held for 4 hours and then removed and held for an additional 24 hours at 4° C. to produce freeze-dried samples. The survival rate of the E. coli JM109 at this point was 26.8% for the sample frozen with liquid nitrogen and 39.1% for the sample not frozen with liquid nitrogen.

[0090] E. coli JM109 has 514 million base pairs of DNA, and .sup.15N-labeling of this DNA was carried out by two methods. In one method, E. coli JM109 is cultured, without the introduction of the glutamine synthetase inhibitor MSX, on a culture medium containing .sup.15N-labeled ammonium ion, and all the nitrogen within the cell, including proteins and nucleic acids, is labeled with .sup.15N (sample F). In the other method, E. coli JM109 is cultured, with the introduction of MSX and .sup.15N-unlabeled glutamine, on a culture medium containing .sup.15N-labeled deoxynucleotides, to yield a biological sample in which only the DNA and RNA is .sup.15N-labeled (sample D).

[0091] Proton beam irradiation samples were produced by preparing three solutions from the two types of .sup.15N-labeled E. coli JM109 and from .sup.15N-unlabeled E. coli JM109 (sample E). The E. coli concentration, dripped amount of solution, dripped area, number of dripped cells, the area density of cells, and .sup.15N area density for each irradiation sample are as follows.

[0092] [Sample D]

[0093] E. coli concentration: 3.17×10.sup.8 cells/mL, dripped amount of solution: 10 μL, dripped area: 1.26 cm.sup.2, number of dripped cells: 3.17×10.sup.6 cells, area density of cells: 2.52×10.sup.6 cells/cm.sup.2, and .sup.15N area density: 9.50×10.sup.13 cm.sup.−2.

[0094] [Sample E]

[0095] E. coli concentration: 3.17×10.sup.8 cells/mL, dripped amount of solution: 10 μL, dripped area: 1.20 cm.sup.2, number of dripped cells: 3.17×10.sup.6 cells, area density of cells: 2.64×10.sup.6 cells/cm.sup.2, and .sup.15N area density: 3.66×10.sup.11 cm.sup.−2.

[0096] [Sample F]

[0097] E. coli concentration: 8.62×10.sup.7 cells/mL, dripped amount of solution: 20 μL, dripped area: 1.56 cm.sup.2, number of dripped cells: 1.72×10.sup.6 cells, area density of cells: 1.11×10.sup.6 cells/cm.sup.2, and .sup.15N area density: 4.18×10.sup.13 cm.sup.−2.

[0098] The amount of 4.43 MeV γ-radiation counted at the same time as proton beam irradiation showed that the ratio of the amount of .sup.15N for the .sup.15N-labeling of only DNA and RNA in sample D was 1 to 44.6 for the case in which the nitrogen in the entire cell in sample F was labeled with .sup.15N.

EXAMPLE 3

Results of Proton Beam Irradiation of .SUP.15.N-Labeled Drug-Resistance Gene Plasmid Samples

[0099] (1) pUC4-KIXX Plasmid and Method for Producing Same

[0100] The gene structure of the pUC4-KIXX plasmid (plasmid DNA) is shown in FIG. 12. This plasmid is a cyclic plasmid (3,853 base pairs (bps)) provided by the insertion of a kanamycin-resistance gene (Kanamycin-R, 1,248 bps) into the pUC4 gene (2,605 bps), which has Ori and an ampicillin-resistance gene (Ampicillin-R). The gene size taken up by the promoter and transcription region for the two drug-resistance genes is 934 bps for the ampicillin-resistance gene and 953 bps for the kanamycin-resistance gene, and the Ori region required for plasmid replication is 621 bps. The base pair types and number of .sup.15N (100% substitution) for each gene region are given in Table 2.

TABLE-US-00002 TABLE 2 .sup.15N labeled pUC4-KIXX plasmid DNA Base Ampicillin − R Ori Kanamycin − R Other area Total pairs (bps)* .sup.15N (bps) .sup.15N (bps)* .sup.15N (bps) .sup.15N (bps) .sup.15N A-T 233 1631 136 952 263 1841 366 2562 998 6986 T-A 254 1778 148 1036 289 2023 307 2149 998 6986 C-G 233 1864 177 1416 189 1512 312 2496 911 7288 G-C 214 1712 160 1280 212 1696 360 2880 946 7568 Total 934 6985 621 4684 953 7072 1345 10087 3853 28828 *promotor + coding area

[0101] A plasmid containing .sup.15N at its natural abundance and a plasmid containing ≥98% .sup.15N were produced using the following method. 250 mL of M9 minimal medium in which the nitrogen source was NH.sub.4Cl containing .sup.15N at its natural abundance (0.364%) was prepared. 250 mL of M9 minimal medium in which the nitrogen source was .sup.15NH.sub.4Cl containing ≥98% .sup.15N was also prepared. Specifically, each of these M9 minimal media was prepared by dissolving Na.sub.2HPO.sub.4 (15 g), KH.sub.2PO.sub.4 (7.5 g), NaCl (1.25 g), NH.sub.4Cl (2.5 g), 1 M (mol/L) MgSO.sub.4 (250 μL), 20% (w/v) glucose 2.5 mL, and 1 M CaCl.sub.2 (25 μL) in 250 mL of ultrapure water, followed by autoclaving and then cooling to room temperature and then the addition of 250 μL of 1% thiamine-HCl. E. coli (JM109) holding the pUC4-KIXX plasmid was cultured on each of these culture media. Specifically, 25 μL of the E. coli was added to the M9 minimal medium, and shake culture was carried out for 2 days at 37° C. and 200 rpm. The E. coli was then recovered, and plasmid purification was carried out using a Plasmid Midi kit (Qiagen) plasmid extraction kit. The plasmids were dissolved in sterile water, and the DNA concentration was quantitated with a NanoDrop (Thermo Fisher Scientific Inc.) fluorometer and adjusted to a concentration of 115 ng/μL. .sup.14N_pUC4_KIXX, a plasmid containing .sup.15N in its natural abundance, and .sup.15N_pUC4-KIXX, a plasmid containing .sup.15N at ≥98%, were produced using this procedure.

[0102] (2) Proton Beam Irradiation of pUC4-KIXX Plasmids

[0103] For each of the two plasmid samples, 1 μL was dripped onto an Si wafer substrate followed by drying, placement in the vacuum chamber, and irradiation of the sample with a proton beam. Proton beam irradiation was carried out using the 1 MV tandem electrostatic accelerator at the Research Facility Center for Science and Technology of Tsukuba University. The proton beam irradiation conditions were the same as in (2) of Example 2. The resonance curve for the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction of the .sup.15N_pUC4-KIXX plasmid sample is given in FIG. 13. The resonance curve acquired for the .sup.15N-labeled deoxyribonucleotide .sup.15N-labeled dGTP is also shown for reference. Proton beam irradiation was carried out by dividing the proton energy into three beam levels in 4 keV steps between 890 keV and 906 keV. The three irradiation levels are given in Table 3.

TABLE-US-00003 TABLE 3 Energy Irradiation Irradiation Total irradiation Sample (KeV) time (s) dose (μC) dose (μC) {circle around (1)} 15N_pUC4- 890 435 0.5005 2.5524 KIXX 894 434 0.5004 898 437 0.5005 902 441 0.5005 906 488 0.5505 {circle around (2)} 15N_pUC4- 890 889 1.0006 5.0533 KIXX 894 879 1.0504 898 828 1.0009 902 835 1.0005 906 860 1.0009 {circle around (3)} 15N_pUC4- 890 1658 2.0002 10.001 KIXX 894 1541 2.0003 898 1477 2.0003 902 1857 2.0001 906 1939 2.0001 {circle around (4)} 14N_pUC4- 890 438 0.5003 2.5015 KIXX 894 441 0.5001 898 454 0.5004 902 458 0.5002 906 467 0.5005 {circle around (5)} 14N_pUC4- 890 850 1.0005 5.0028 KIXX 894 820 1.0004 898 799 1.0005 902 803 1.0005 906 822 1.0009 {circle around (6)} 14N_pUC4- 890 1904 2.0003 10.0012 KIXX 894 1799 1.9999 898 1733 2.0003 902 1739 2.0005 906 1834 2.0002

[0104] (3) Transformation with Proton Beam-Irradiated Plasmids

[0105] 8.6 ng of the proton beam-irradiated plasmid was added to 50 μL of E. coli (1×10.sup.10 cells/mL), and the plasmid was introduced into the E. coli cells by electroporation. The electroporation process was run for a current passage interval of 3.5 to 3.7 ms using a direct-current field, a voltage of 1,500 V, a resistance of 200 Ω, and a capacitance of 25 μF. 1 mL of LB medium was added and shaking culture was carried out for 1 hour (37° C., 200 rpm). During this culturing process, the plasmids, that were damaged by proton beam irradiation with cleavage of the circular form to be a linear shape, were not replicated in the E. coli cells, and as a consequence, of the proton beam-irradiated plasmids, only the plasmids that retained the circular form were amplified with the occurrence of transformation.

[0106] (4) Evaluation of the Degree of Damage to Drug-Resistance Genes

[0107] Three types of culture plates with the addition of the two drugs were prepared. A 100 μL aliquot of E. coli transformed with proton beam-irradiated plasmid was seeded to each of the following culture plates and the number of colonies formed was analyzed: (a) 100 μg/mL ampicillin, (b) 50 μg/mL kanamycin, (c) 100 μg/mL ampicillin+50 μg/mL kanamycin. As a control sample, a 100 μL aliquot with the unirradiated plasmid was also seeded to the three culture plates to which the drugs had been introduced in the same manner. The numbers of colonies appearing on the three drug-added culture plates are given in FIG. 14, FIG. 15, and FIG. 16. The vertical axis shows values normalized by the number of colonies appearing for the control sample (=1.0), and the average value for three measurements is given. The upper limit and lower limit on the results of the three measurements are given for the error. The colony generation count at 10 μC was 0 in each figure, but the value of the detection limit is plotted in the figures. The vertical axis shows the fraction that functions normally in the absence of damage to the two drug-resistance genes in the plasmid by proton beam irradiation. At a total irradiation dose of 2.5 μC, it is shown that the .sup.15N_pUC4-KIXX plasmid receives greater irradiation damage in excess of the error. This result shows that the .sup.15N(.sup.1H, α.sub.1γ).sup.12C resonant nuclear reaction imparts substantial damage to genes in excess of the ionization effects of the proton beam. It is considered that the genes receive nonspecific damage when the total irradiation dose in FIG. 14 reaches about 5.0 μC or higher.

[0108] The embodiments described in the preceding have the purpose of facilitating an understanding of the present invention and are not intended to limit the interpretation of the present invention. The individual elements provided in the embodiments, as well as their positions, materials, conditions, shapes, sizes, and so forth, should not be construed as being limited to that which has been provided as exemplary and may be modified as appropriate. In addition, the structures shown in different embodiments may be partially replaced by or combined with each other.