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1. Mies F.H., Phys. Rev. 175 164 (1968). 

2. =_ee_jXB@WLN 

3. Heller Y.I., Phys. Lett. 82A 4 (1981). 

4. Bachau H., Phys. Rev. A 34 4785 (1986). 

5. Karapanagioti N.E., Phys. Rev. A 53 2587 (1996). 

6. Magunov A.I., Rotter I., Strakhova S.I. J. Phys. B: At. Mol. Opt. Phys., 32, 1669 (1999). 

7. Fano U., Phys. Rev 178 131 (1969). 

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gh-hlebiZl_evgucj_`bf]hj_gbyjZajy^Zdh]^ZijbebiZgb_we_dljhgh\dfhe_dmeZf 

O 2 ijZdlbq_kdbiheghklvxmjZ\gh\_rb\Z_lkybohlebiZgb_fgZO( 3 PbO 2 (a 1 û g IhdZ 

aZghqlh\^Zgguomkeh\byohkgh\gufhljbpZl_evgufbhghfy\ey_lkybhgO - :gZeba 

^bgZfbdb]b[_ebbhgh\O - ^Ze\hafh`ghklv\i_j\u_g_ihkj_^kl\_ggh\kZfhcieZaf_ 

hij_^_eblvdhgklZglukdhjhklbijhp_kkh\ZkkhpbZlb\gh]hhlebiZgbygZZlhfZoO( 3 P) 

− 3 

( O + O( P) 

→ O + e : k O d =(1.9±0.4)⋅10 -10 kf 3 k b fhe_dmeZo O 2 (a 1 û g ) 

2 

− 

( O + O ( a 

1 

2 

∆ 

g 

) → products + e : k ∆ d =(1.4±0.3)⋅10 -10 kf 3 k. 

Hkh[mxp_gghklvij_^klZ\ey_llhqlh\k_\_ebqbgug_h[oh^bfu_êyhij_^_ 

e_gby^ZgguodhgklZgl[uebihemq_guwdki_jbf_glZevghDjhf_lh]hwlb\_ebqbgu 

hljbpZl_evgu_bhguZlhfubkbg]e_lgu_fhe_dmeudbkehjh^Zbaf_jyebkv\©h^ghcª 

ijhkljZgkl\_gghc lhqd_ Wlh kms_kl\_ggh hlebqZ_l gZrb baf_j_gby hl ij_û^msbo 

jZ[hl>@Ihwlhfmohl_ehkv[uihj_dhf_g^h\Zlvhij_^_e_ggu_\^ZgghcjZ[hl_dhg 

klZglukdhjhklb]b[_ebhljbpZl_evguobhgh\H – gZZlhfZoO( 3 Pbfhe_dmeZoO 2 (a 1 û g ) 

êybkihevah\Zgby\[ZaZo^Zgguoêyfh^_ebjh\ZgbyieZafu 

[1] Lieberman M.A., Lichtenberg A.J. Principles of Plasma Discharges and Material Process 

ing. New York: Wiley, 1994. 

[2] Ramamurthi B., Economou D.J. // J. Vac. Sci. Technol. A, 2002, Vol.20, No. 2, pp. 467- 

478. 

[3] Panda S., Economou D.J. // J.Appl. Phys., 2000, Vol. 87, No. 12, pp. 8323-8333. 

[4] Fehsenfeld F.C., Albritton D.L., Burt J.A., Schiff H.I.// Can.J.Chem., 1969 Vol.47, 

p.1793. 

[5] Upschulte B.L., Marinelli W.J., Green B.D.// J.Phys.Chem., 1994, Vol.98, pp.837-842. 

GBFL:KL:;BEVGUOMJH


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AZibr_f\ujZ`_gb_êydhgklZgluJηΣ 0 Σ 0 \\b^_ 

g(ηΣ 0 Σ 0 ) = g ηuu F+g ηdd F+g ηss (F-D) = -g ηss D =√(2/3)D. 

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g(ηΣ 0 usΣ 0 us) = -g ηuu D=-√(1/6)D 

b (d ⇔ s) 

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] 

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k\yabΣ 0 : 

√(1/2) m 2 η λ 2 Σ g(ηΣ 0 Σ 0 ) exp(-m 2 Σ /M 2 ) [1+A Σ M 2 ] = 

= m 2 η M 4 E0(x) [g ηss /12/π 2 /f η +3f 3η /4/f η /√(2)-M 2 /f η [g ηss [m d + 

m u ]- m 2 η /72/ f η [g ηss ] 

+ m 2 0 /6/ f η [ (g ηuu m d +g ηdd m u )] ≡ D(u,d,s) 

28


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pbZpbb CHF 3 we_dljhgguf m^Zjhf :[khexlgh_ agZq_gb_ ihegh]h k_q_gby ^bkkhpbZ 

pbbihemq_ghgZfbijbghjfbjh\d_gZwdki_jbf_glZevgu_^Zggu_ihbhgbaZpbhgghfm 

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i_jbf_glZevgufb^ZggufbdZd\qbklhfCHF 3 lZdb\kf_kbCHF 3 :Arblh]h\ucgZ[hj 

k_q_gbcfh`_l[ulvbkihevah\Zgijbqbke_gghffh^_ebjh\Zgbbwe_dljhgghcdbg_lbdb 

\jZaebqguoieZaf_gguoj_ZdlhjZo 

1. Morgan L., Winstead C. and McKoy V. // J. Appl. Phys., 2001, v.90, p.2009 

2. Kushner M.J. and Da Zhang // J. Appl. Phys., 2000, v.88, p.3231 

3. Wang Y., Christophorou L.G. et al // Chem. Phys. Lett, 1999, v.304, p.303 

4. Christophorou I.G. Olthoff J.K. et al // J. Phys. Chem. Ref. Data, 1997, v.26, p.1 

5. Goto M., Nakamura K., Toyoda H. and Sugai H. // J. Appl. Phys., 1994, v.33, pp.3602- 

3607 

6. Phelps A.V., JILA Information Center Report N28, 1985 

31

32 

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2. :]Znhgh\:

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2. >`;ZdZeG_cljbggZyZkljhnbabdZFhkd\ZBa^-\h©Fbjª. 

3. Borexino Collaboration «Science and technology of borexino: a real time detector for low 

energy solar neutrinos» // Astroparticle Physics, November 27, 2000. 

35

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>@^ZgguoKZde_êyj_Zdpbc(γ,xn), (γQbγ,2n). 

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gu_\aZbfghkh]eZkh\Zggu_^Zggu_ihk_q_gbyfj_ZdpbcγQêyy^_j 117 Sn, 118 Sn, 

119 Sn, 124 Sn, 127 I, 133 Cs, 159 Tb, 165 Ho, 181 Ta, 197 Au, 208 3Ebijh\_^_ghkjZ\g_gb_ihemq_gguo 

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g_ggufb\wdki_jbf_glZobgh]hlbiZ–gZimqdZolhjfhagh]hγ-baemq_gbyijbbkihev 

ah\Zgbbf_lh^ZgZ\_^_gghcZdlb\ghklb>@ 

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03-07-b‹ 04-02-16275. 

1. Fuller E.G., Gerstenberg H. Photonuclear Data - Abstracts Sheets 1955 - 1982. NBSIR 

83-2742. U.S.A. National Bureau of Standards, 1983. 

2.


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1. EZchgk E Mbevyfk > NbabdZ fZ]gblhkn_ju Dhebq_kl\_gguc ihôh^ F Fbj 

k 

2. Gbrb^Z:=_hfZ]gblguc^bZ]ghaZlfhkn_juFFbjk 

3. Sergeev V.A., Sazhina E.M., Tsyganenko N.A. Pitch-angle scattering of energetic protons 

in the magnetotail current sheet as the dominant source of their isotropic precipitation into 

the nightside ionosphere // Planet Space Sci., 1983, vol. 31, 10, p. 1147-1155. 

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1. ;ZjZgh\ B: P_i_e_\bq KH Y\ebgkdbc XG G_mijm]h_ jZkiue_gb_ l\_jûo 

l_eMNGl‹k-510. 

2. Toulemonde M. Nanometric phase transformation of oxide materials under GeV energy 

heavy ion irradiation.// Nucl. Instr. and Meth. in Phys.Res. B 1999, v‹-4, p .1-11. 

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1. Collins F.S., Green E.D., Guttmacher A.E., Guyer M.S. Nature 422, 835. 

2. Hamai C., Tanaka H., and Kawai T. J. Vac. Sci. Technol. B 17, 1313. 

3. Gerritsen J.W., Elemans J.A.A.W., Hulsken B., Travaille A.M., Kempen H. van, Rasing 

Th., and Speller S. AIP Conference Proceedings 696, 365. 

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1. Walker, D.A. Photosynth. Res. 1992. 34. P. 387-395. 

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1. Tarasova O.A., A.Yu. Karpetchko, Accounting for local meteorological effects in the 

ozone time-series of Lovozero (Kola Peninsula), Atmos. Chem. Phys., 3, 2003, p. 941-949. 

2. LZjZkh\Z H: Dmag_ph\ =B eZgkdbc GN K_gbd B: Kf_lgbd B $ Hkh 

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rbjbgudeZjfhjh\kdhfmjZ^bmkmbhgh\ 

1. Sonnerup B.U.O. “Adiabatic particle orbits in magnetic null sheet” // J. Geophys. Res., 

1971, v. 76, p. 8211. 

2. Chen J. and Palmadesso P.J. “Chaos and nonlinear dynamics of single-particle orbits in 

magnetotaillike magnetic field” // J. Geophys. Res, 1986, v. 91, p. 1499 

3. Hoshino M., Nishida A., Mukai T., Saito Y., and Yamamoto T. “Structure of plasma sheet 

in magnetotail: double-peaked electric current sheet” // J. Geophys.Res., 1996, v. 101 p. 

24775. 

4. Asano Y., Mukai T., Hoshino M., Saito Y., Hayakawa H., and Nagai T. “Evolution of the 

thin current sheet in a substorm observed by Geotail” // J. Geophys. Res.,2003, v. 108, p. 

10101.

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MEVLJ:A

104 

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< gZklhys_c jZ[hl_ bkke_^m_lky \hafh`ghklv ijbf_gbfhklb h^ghklZ^bcguo 

ko_fJha_g[jhdZdkbkl_fZf\b^Z 

dzl 

= Gl( z1, z2,... zN) 

, l = 1,.. N 

(3) 

dt 

N 

A^_kv z = ( z , z ,..., z ) ∈C 

Z g = g ( z , z ,..., z ) ∈ C ∞ –ZgZeblbq_kdb_ nmgdpbb dhfie_dk 

1 2 

N 

l l 1 2 N 

guoi_j_f_gguo z 1 

, z 2 

,..., z 

N 

. 

>Ze__[m^_fbkihevah\Zlvko_fmJha_g[jhdZ>@kdhfie_dkgufdhwnnbpb_glhf 

aZibkZggmx\nhjf_ijb]h^ghcêydhfie_dkghagZqguoH>M 

zˆ = z+ 0.5 ⋅τ( υ+ w) , ⎡⎣E− 0.5( 1 + i) τGz⎤⎦υ= f ( z, t+ 0.5 τ) , ⎡⎣E−0.5( 1 −i) τ Gz⎤⎦ w= f ( z, t+ 0.5 τ) 

. (4) 

A^_kv Gz 

≡∂G ∂ z –fZljbpZYdh[b E –_^bgbqgZyfZljbpZ τ –rZ]ih\j_f_gb z –j_ 

r_gb_gZl_dms_f\j_f_gghckeh_ ẑ –j_r_gb_gZgh\hf\j_f_gghfkeh_LZdbfh[jZ 

ahf êy i_j_oh^Z gZ ke_^mxsbc \j_f_gghc kehc lj_[m_lky ^\Z`û j_rblv kbkl_fm 

ebg_cguomjZ\g_gbcGhfZljbpukbkl_f\(4)ohjhrhh[mkeh\e_gubj_r_gb_ke_^m_l 

\uihegylv ijyfufb f_lh^Zfb L_f kZfuf i_j_oh^ \uihegy_lky aZ dhg_qgh_ aZjZg__ 

ba\_klgh_qbkeh^_ckl\bcdZd\y\guoko_fZoKo_fZ(4)h[eZ^Z_lmgbdZevgufbk\hc 

, L2 –mklhcqb\hklvbkhhl\_lkl\_ggh[_amkeh\gZymklhcqb 

2 

kl\Zfb>@lhqghklv O( τ ) 

\hklvWlZko_fZh[eZ^Z_l\ukhdhcgZ^_`ghklvxbijb]h^gZêyjZkq_lZaZ^Zqkkbev 

ghc`_kldhklvxBf_gghwlZko_fZbkihevah\ZgZ\hibkZgguogb`_jZkq_lZoaZwlhc 

ko_fhc\ebl_jZlmj_aZdj_ibehkvgZa\Zgb_ko_fZCROS. 

>ey beexkljZpbb \hafh`ghklb ijbf_gbfhklb ko_fu &526 d kbkl_fZf dhf 

ie_dkguo ^bnn_j_gpbZevguo mjZ\g_gbc [ue\ayl ijbf_jbanbabdb]hj_gby < 

]h^m Kb\Zrbgkdbc>@ihdZaZe qlh ^bgZfbdZ njhglZ ieZf_gb fh`_l [ulv hibkZgZ k 

ihfhsvxg_ebg_cgh]hmjZ\g_gby\qZklguoijhba\h^guokh^_j`Zs_]hik_\^h^bnn_ 

j_gpbZevguchi_jZlhj 

ut + uux =Λ u+ vuxx, (5) 

]^_hi_jZlhj Λ hij_^_ey_lkyq_j_aij_h[jZah\Zgb_Nmjv_ihijhkljZgkl\_gghci_j_ 

f_gghc 

+∞ +∞ 

 

 

u t x e u t k dk u t x e k u t k dk. 

( , ) ikx 

ikx 

= ( , ) ; Λ ( , ) = ⋅ ( , ) 

∫ 

−∞ 

MjZ\g_gb_Kb\Zrbgkdh]hh[eZ^Z_lbgl_j_kgufk\hckl\hfdhlhjh_h[uqghgZ 

au\ZxliheyjgufjZaeh`_gb_fpole decompositionZbf_gghmjZ\g_gb_(5)^himkdZ_l 

j_r_gby\\b^_>@ 

2N 

1 

u( t, x) 

=−2ν∑ (6) 

x−z t 

∫ 

−∞ 

α= 1 α 

]^_ z α 

ihexkZgZdhfie_dkghciehkdhklbijbqzfihexkZijbkmlkl\m_l\nhjfme_ (6) 

dhfie_kghkhijy`zggufb iZjZfb >\b`_gb_ihexkh\ijhbkoh^blihke_^mxs_fmaZ 

dhgm 

1 

z α 

=−2ν∑ 

−i⋅sign( Imzα) 

. (7) 

z −z 

β≠α α β 

< kemqZ_ 2π-i_jbh^bqghklbihijhkljZgkl\_gghci_j_f_gghcfh`ghjZkkfZl 

jb\ZlvlhevdhihexkZkj_ZevghcqZklvx Re z α 

∈( 0,2π) 

b\f_klhmjZ\g_gbc(6)b(7)bk 

ihevah\Zlvke_^mxsb_mjZ\g_gby 

()

106 

EHFHGHKH


4. Thual O., Frich U., Henon M. Application of pole decomposition to an equation governing 

the dynamics of wrinkled flame fronts // J. Physique 46 (1985) 1485-1494. 

M>D14 

>B:=GHKLBD:HKH;GGHKLCJRGBY 

IJBJ:KQL:OKOFHCCROS 

** :evrbgZ: 1 DZebldbgGG 1 DhjydbgI< 2 

1 BgklblmlfZl_fZlbq_kdh]hfh^_ebjh\ZgbyJ:G 2 Fhkdh\kdbc]hkm^Zjkl\_gguc 

bgklblmlwe_dljhgghcl_ogbdbL_ogbq_kdbcmgb\_jkbl_l 

JZkkfhljbfaZ^ZqmDhrbêyh[udgh\_ggh]h^bnn_j_gpbZevgh]hmjZ\g_gby 

11 + β 

u′ t =βu ; t ≥ 0; u 0 = u . (1) 

Lhqgh_j_r_gb_bf__l\b^ 

() ( ) 

0 

= ( − ) 

−β 

= . (2) 

ut ( ) t t ; t 1 u 

* * 0 

>ey β> 0 lhqgh_j_r_gb_l_jibljZaju\\lhjh]hjh^Zijb t * 

bg_kms_kl\m 

_lijb t > t* 

. 

kebj_rZlvmjZ\g_gb_qbke_gghihy\ghcko_f_Jmg]_-DmllZlhqghklb Oτ () 

ERK lh qbke_ggh_ j_r_gb_ [m^_l \k_]^Z iheh`bl_evguf b fhghlhggh \hajZklZx 

sbf 

2 

u = u( 0 ); u = u+τ u , n= 0,1,...; tn 

= nτ (3) 

0 

ˆ 

Ijbwlhfgbqlhg_]h\hjblh[hkh[_gghklbj_r_gby\lhqd_ t * 

bkoh^yba\b^Z 

fh`ghk^_eZlv\u\h^qlhj_r_gb_kms_kl\m_lijbex[uo t n 

GZijZdlbd_ijbf_ 

g_gb_ko_fuijb t →∞ijb\h^bldi_j_iheg_gbxkq_lZZijbqbgZi_j_iheg_gby 

hklZzlky g_ba\_klghc :gZeh]bqgh_ dZq_kl\_ggh_ ih\_^_gb_ qbke_ggh]h j_r_gby êy 

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@dhlhjuc 

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kemqZ_kl_i_gghchkh[_gghklb\b^Zfh`ghmklZgh\blvihjy^hdihexkZ β Ihkljh_ 

gZlZd`_^bZ]ghklbdZjZaju\h\\ukhdboijhba\h^guolhqgh]hj_r_gby:\lhjZfbih 

dZaZghqlhijbf_g_gb_ko_fuCROSbagZqZevghij_êh`_gghcêy`_kldboaZ^Zqg_ 

ijb\h^bldi_j_iheg_gbxjZkq_lh\biehohh[mkeh\e_gguoaZ^Zq 

H^ghiZjZf_ljbq_kdh_ k_f_ckl\h h^ghklZ^bcguo ko_f Jha_g[jhdZ êy mjZ\g_ 

gby 

u′ t = F u, 

t 

() ( ) 

hibku\Z_lkyke_^mxsbfnhjfmeZfb 

u = u 0 ; u = u+τRe k; E−ατ∂F ∂ u k = F u, t+ 0.5τ . (4) 

( ) ( ) ( ) 

0 

ˆ 

** >hdeZ^hlf_q_g`xjbdZdh^bgbaemqrbogZih^k_dpbb

108 

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]_[jZbq_kdbo mjZ\g_gbc k fZljbp_c ( E−ατ∂F ∂u) 

Lh _klv i_j_oh^ gZ gh\uc kehc 

dZdb\y\guo ko_fZoijhbkoh^blaZdhg_qgh_aZjZg__ba\_klgh_qbkehrZ]h\LZdb_ 

ko_fu gZau\Zxlky y\gh-g_y\gufb Kms_kl\m_l h^gZ ko_fZ CROS ba k_f_ckl\Zk 

2 

dhfie_dkgufiZjZf_ljhf α= ( 1+ i) 

2mgbdZevgufbk\hckl\Zfblhqghklv 

O( τ ), L2- 

mklhcqb\hklv fhghlhgghklvxgZebg_cguoaZ^ZqZobbkdexqbl_evgZygZ^_`ghklvgZ 

`_kldboaZ^ZqZo 

Dhgljhev lhqghklb f_lh^hf k]ms_gby k_ldb ij_êh`_g _s_ JbqZj^khghf \ 

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N b rN maeZfbih]j_rghklvqbke_ggh]hj_r_gby\kh\iZ^ZxsbomaeZok_lhd\uqbk 

ey_lkyihZkbfilhlbq_kdblhqghcijb N →∞nhjfme_ 

( rN ) ( N ) 

( rN ) u −u 

−p 

∆ () t = + o 

p ( N ) 

(5) 

r −1 

]^_p –l_hj_lbq_kdbcihjy^hdlhqghklbko_fu 

2 

Ihj_amevlZlZfjZkqzlh\gZljzok_ldZoNrNrNfh`gh\uqbkeblvwnn_d 

, , 

lb\gucihjy^hdlhqghklbko_fu 

( N) ( rN) 

eff ln ∆ −ln 

∆ 

p () t = . 

(6) 

ln r 

F_lh^bdZ ^bZ]ghklbdb kbg]meyjghklb gZ hkgh\_ f_lh^Z k]ms_gby k_ldb b ijb 

jZkq_lZoko_fhcCROS[Zabjm_lkygZke_^mxsbo^hdZaZgguoZ\lhjZfbml\_j`^_gbyo 

Ml\_j`^_gb_ 1. Kms_kl\m_l agZq_gb_ u = ⎡ 

β 

∗ ⎣2 τ ( β+ 1) 

⎤ ⎦ , ijbdhlhjhfqbke_ggh_ 

j_r_gb_ko_fu&526êyaZ^Zqbg_f_gy_lkyijbi_j_oh^_gZke_^mxsbc\j_f_g 

ghckehc û : û = u ∗ 

. 

Ml\_j`^_gb_ k\hckl\h ijbly`_gby. Ijb u > u ∗ 

ijbjZs_gb_ nmgdpbb 

uˆ − u < 0 bgZh[hjhlijb u 

ijbjZs_gb_nmgdpbb uˆ − u > 0 . L_ijbex[hfagZq_ 

gbb u gZl_dms_f\j_f_gghfkeh_ke_^mxsbcrZ]ko_fZ&526^_eZ_lihgZijZ\e_ 

gbxdiheh`_gbxjZ\gh\_kby u = ⎡ 

β 

∗ ⎣2 τ ( β+ 1) 

⎤ ⎦ . 

Ml\_j`^_gb_ Ijbhkh[_gghklblhqgh]hj_r_gbyH>MlbiZihexkZ β> 0 

qbke_ggh_ j_r_gb_ ko_fu CROS klj_fblky dij_^_em u ∗ 

. Ijbhkh[_gghklblbiZdhjgy 

−1≤β< 0 qbke_ggh_j_r_gb_ko_fu&526klZ[bebabjm_lky\ihehk_\hdjm]iheh`_ 

gbyjZ\gh\_kby u ∗ 

. 

>eyH>Mlhqgh_j_r_gb_dhlhjh]hbf__lhkh[_gghklv\b^Z u ln( t t) 

∗− kijZ 

\_êb\uml\_j`^_gby 

Ml\_j`^_gb_ Kms_kl\m_liheh`_gb_jZ\gh\_kby u ∗ 

= ln τ− ln 2 , ijbdhlhjhf 

qbke_ggh_j_r_gb_ko_fu&526g_f_gy_lkyijbi_j_oh^_gZke_^mxsbc\j_f_gghc 

kehc 

Ml\_j`^_gb_ 5. Ijb u > u ∗ 

ijbjZs_gb_ nmgdpbb uˆ − u < 0 b gZh[hjhl ijb 

u

ijbjZs_gb_nmgdpbb uˆ − u > 0 . 

Ml\_j`^_gb_ 6.


Ml\_j`^_gby iha\heyxlmklZgh\blvihjy^hd β ijbkl_i_gghchkh[_gghklb 

() ( − ) beb^bZ]ghklbjh\Zlveh]Zjbnfbq_kdmxhkh[_gghklv u() t ln ( t t) 

u t t* 

t −β 

* 

− . 

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u() t ( t* 

− t) 

−β 

eff 

\ maeZo t ≥ t* 

wnn_dlb\guc ihjy^hd lhqghklb ko_fu &526 p →−β 

1 

ijb τ N − → 0 . 

Ml\_j`^_gb_ Ijb gZebqbb kbg]meyjghklb lhqgh]h j_r_gby lbiZ 

u() t ln ( t* 

− t) 

\maeZo t ≥ t* 

ih]j_rghklv ko_fu CROS ( N ) ln r 

−p 

∆ () t =− + o 

p ( N ), Z 

r −1 

eff 

1 

p → 0 ijb τ N − → 0 . 

;ueb ijh\_^_gu fgh]hqbke_ggu_ l_klh\u_ jZkq_lu k jZaebqguf lbiZfb hkh 

[_gghkl_clhqgh]hj_r_gbyEBJH:JGHCHFKLJEV;U 

Ohoeh\:: 

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>IDhklhfZjh\ fbljb_\ F=M Ljmû nZdmevl_lZ


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k]jZgbqgufbmkeh\byfbG_cfZgZgZ]jZgbpZoihehku ∂ Ω= { y =0 , y = 1} 

: 

∂u 

= 0 

∂n 

∂Ω 

(2) 

bmkeh\bx 

u ∈ L 2( 

Ω ) 

(3) 

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mathematics and physics in secondary and higher education. Proceedings of the Third Inter-Karelian 

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2. ;Zjur_\:D 537.874.23 

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148 

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jZ\_gWlh lZd gZau\Z_fuc wnn_dl g_\b^bfdb


4. Plihal M., Shambrook A., Maradudin A.A. “Two-dimensional photonic band structures”, 

Optics Communications, vol. 80, No. 3, 1 January 1991. 

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2. :ofZgh\K:GbdblbgKXNbabq_kdZyhilbdZBa^Zl_evkl\hFhkdh\kdh]hmgb 

\_jkbl_lZk-b-346. 

3. EZg^k[_j]=KHilbdZFhkd\Zk-103. 

4. Iskhakov T.Sh., Ivanova O.A. and Chekhova M.V. "Multi-photon states and their measurement" 

// Proceedings of the Second International Symposium Quantum Informatics, 

October 5-8 2004, Moscow, Proceedings of SPIE, 2005. 

5. Brown R., Hanbury R.Q. and Twiss R.Q., 1964, Nature, London, 177, 27. 

6. Haner A.B. and Isenor N.R. "Intensity Correlations from Pseudothermal Light Sources" // 

American Journal of Physics, June 1970, volume 38, number 6, p. 748-751. 

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x 

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1. Kivshar Y.S., Ostrovskaya E.A. // Optics&Photonics News. 2002. V. 2. P. 28. 

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in active media // Proceedings of SPIE, 2001, v. 4644, P. 312-318. 

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903-908. 

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1. Handbook of Optical Coherence Tomography, Bouma B.E., Tearney G.J., eds. (New 

York, Marcel Dekker, 2002). 

2. Wang R.K. Signal degradation by multiple scattering in optical coherence tomography of 

dense tissue: a Monte Carlo study towards optical clearing of biotissues, Phys. Med. Biol. 

47, 2281-2299 (2002). 

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2. Loskutov A., Rybalko S. and Zhuchkova E. Model of cardiac tissue as a conductive system 

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Philadelphia, 1995. 

5. Dh\Ze_\ZG.:., Ehkdmlh\:.X. >:G, 2004, f 396, No 1. 

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anisoplanatism in adaptive optics, JOSA A Vol. 15, No 8, 2097-2106, 1998. 

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1. Kaesarmann F., Kempf Ch. Buckminsterfullerene and Photodynamic Inactivation of Viruses. 

Reviews in Medical Virology 1998, 8, 143-151


2. Da Ros T., Spallutto G., Prato M. Biological Applications of Fullerene Derivatives:A 

Brief Overview. Croatical Chemica Acta. 2001, 74 (4), 743-755 

3. Scharff P., Risch K., Carta-Abelmann L., Dmytruk I., Bilyi M., Golub O., Khavryuchenko 

A., Buzaneva E., Aksenov V., Avdeev M., Prylutskyy Yu., Durov S. Structure of C 60 

fullerene in water: spectroscopic data. Carbon, 2004, 42(5-6), 1203-1206 

4. Heymann D., Bachilo S., Weisman B., Cataldo F., Fokkens R., Nibbering N., Vis R., Chibante 

F.. C 60 O 3 , a Fullerene Ozonide: Synthesis and Dissociation to C 60 O and O 2 . 

J.Am.Chem.Soc. 2000, 122, 11473-11479 

5. Richard D. Webster and Graham A. Heath, Voltammetric, EPR and UV-VIS-NIR spectroscopic 

studies associated with the one-electron oxidation of and in C 60 C 70 1, 1’, 2, 2’- 

tetrachloroethane containing tri-uoromethanesulfonic acid, Phys. Chem. Chem. Phys., 

2001, 3, 2588 – 2594

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