Literature DB >> 21588948

6-(2-Chloro-benz-yl)-1-(4-chloro-phen-yl)-7-hy-droxy-2,3-dihydro-1H-imidazo[1,2-a]pyrimidin-5-one.

Waldemar Wysocki, Dariusz Matosiuk, Marzena Rządkowska, Zbigniew Karczmarzyk, Zofia Urbańczyk-Lipkowska, Przemysław Kalicki.   

Abstract

The title compound, C(19)H(15)Cl(2)N(3)O(2), was obtained by a one-step cyclo-condensation of 2-amino-1-(4-chloro-phen-yl)imidazoline with diethyl (2-chloro-benz-yl)malonate under basic conditions. In the crystalline state, the mol-ecule exists as the 7-hy-droxy-5-oxo tautomer. The dihedral angles between the fused imidazopyrimidine and aromatic chloro-phenyl and chloro-benzyl rings are 14.2 (1) and 70.7 (1)°, respectively. The conformation of the mol-ecule is influenced by the intra-molecular C-H⋯O and C-H⋯N hydrogen bonds, giving a nearly planar five-ring fused system [maximum deviation from the mean plane = 0.296 (2) Å]. In the crystal structure, strong inter-molecular O-H⋯O hydrogen bonds link the mol-ecules into chains along the c axis. These chains are further stabilized by weak C-H⋯Cl and π-π inter-actions [centroid-centroid distance = 3.6707 (12) Å].

Entities:  

Year:  2010        PMID: 21588948      PMCID: PMC3009369          DOI: 10.1107/S160053681003919X

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background to dioxo derivatives of fused imidazoline ring systems, their biological activity and medical applications, see: Matosiuk, Fidecka, Antkiewicz-Michaluk, Dybała et al. (2002) ▶; Matosiuk, Fidecka, Antkiewicz-Michaluk, Lipkowski et al. (2002 ▶). For the synthesis, see: Rządkowska et al. (2004 ▶). For a related structure, see: Wysocki et al. (2006 ▶). For structure inter­pretation tools, see: Allen et al. (1995 ▶); Allen (2002 ▶); Bruno et al. (2002 ▶). For resonance-assisted hydrogen bonds, see: Gilli et al. (1989 ▶).

Experimental

Crystal data

C19H15Cl2N3O2 M = 388.24 Monoclinic, a = 11.4521 (3) Å b = 12.8287 (4) Å c = 11.7255 (3) Å β = 96.283 (2)° V = 1712.31 (8) Å3 Z = 4 Cu Kα radiation μ = 3.58 mm−1 T = 296 K 0.26 × 0.25 × 0.11 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2005 ▶) T min = 0.415, T max = 0.674 12489 measured reflections 3040 independent reflections 2521 reflections with I > 2σ(I) R int = 0.042

Refinement

R[F 2 > 2σ(F 2)] = 0.039 wR(F 2) = 0.112 S = 1.05 3040 reflections 280 parameters All H-atom parameters refined Δρmax = 0.28 e Å−3 Δρmin = −0.29 e Å−3 Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2005 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053681003919X/fj2343sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S160053681003919X/fj2343Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C19H15Cl2N3O2F(000) = 800
Mr = 388.24Dx = 1.506 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54178 Å
Hall symbol: -P 2ybcCell parameters from 3410 reflections
a = 11.4521 (3) Åθ = 3.9–66.7°
b = 12.8287 (4) ŵ = 3.58 mm1
c = 11.7255 (3) ÅT = 296 K
β = 96.283 (2)°Block, colourless
V = 1712.31 (8) Å30.26 × 0.25 × 0.11 mm
Z = 4
Bruker APEXII CCD diffractometer3040 independent reflections
Radiation source: fine-focus sealed tube2521 reflections with I > 2σ(I)
graphiteRint = 0.042
φ and ω scansθmax = 67.8°, θmin = 3.9°
Absorption correction: multi-scan (SADABS; Bruker, 2005)h = −13→12
Tmin = 0.415, Tmax = 0.674k = −15→8
12489 measured reflectionsl = −13→13
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: difference Fourier map
wR(F2) = 0.112All H-atom parameters refined
S = 1.05w = 1/[σ2(Fo2) + (0.0566P)2 + 0.4965P] where P = (Fo2 + 2Fc2)/3
3040 reflections(Δ/σ)max < 0.001
280 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = −0.29 e Å3
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. Weighted least-squares planes through the starred atoms (Nardelli, Musatti, Domiano & Andreetti Ric.Sci.(1965),15(II—A),807). Equation of the plane: m1*X+m2*Y+m3*Z=dPlane 1 m1 = -0.57842(0.00033) m2 = -0.67971(0.00033) m3 = -0.45102(0.00053) D = -11.68389(0.00244) Atom d s d/s (d/s)**2 N1 * -0.0460 0.0016 - 28.384 805.647 C2 * 0.0029 0.0018 1.594 2.541 N3 * 0.0198 0.0015 13.215 174.625 C4 * -0.0357 0.0023 - 15.771 248.720 C5 * 0.0819 0.0023 36.135 1305.707 N6 * 0.0038 0.0015 2.558 6.543 C7 * 0.0139 0.0017 7.983 63.731 C8 * 0.0007 0.0018 0.384 0.147 C9 * -0.0243 0.0018 - 13.656 186.495 ============ Sum((d/s)**2) for starred atoms 2794.157 Chi-squared at 95% for 6 degrees of freedom: 12.60 The group of atoms deviates significantly from planarityPlane 2 m1 = -0.71141(0.00065) m2 = -0.48107(0.00093) m3 = -0.51231(0.00073) D = -11.40891(0.00306) Atom d s d/s (d/s)**2 C21 * 0.0042 0.0018 2.264 5.124 C22 * -0.0048 0.0022 - 2.159 4.661 C23 * -0.0012 0.0023 - 0.496 0.246 C24 * 0.0051 0.0021 2.408 5.797 C25 * -0.0050 0.0024 - 2.037 4.149 C26 * -0.0018 0.0023 - 0.782 0.611 ============ Sum((d/s)**2) for starred atoms 20.589 Chi-squared at 95% for 3 degrees of freedom: 7.81 The group of atoms deviates significantly from planarityPlane 3 m1 = -0.47124(0.00082) m2 = 0.42681(0.00103) m3 = -0.77186(0.00062) D = -3.90575(0.01406) Atom d s d/s (d/s)**2 C31 * -0.0026 0.0019 - 1.391 1.935 C32 * 0.0016 0.0021 0.757 0.573 C33 * 0.0031 0.0027 1.149 1.321 C34 * -0.0079 0.0031 - 2.556 6.533 C35 * 0.0042 0.0031 1.328 1.764 C36 * 0.0021 0.0024 0.859 0.738 ============ Sum((d/s)**2) for starred atoms 12.865 Chi-squared at 95% for 3 degrees of freedom: 7.81 The group of atoms deviates significantly from planarityDihedral angles formed by LSQ-planes Plane - plane angle (s.u.) angle (s.u.) 1 2 14.18 (0.06) 165.82 (0.06) 1 3 70.69 (0.06) 109.31 (0.06) 2 3 58.31 (0.06) 121.69 (0.06)
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
N10.54690 (14)0.58844 (13)0.65922 (13)0.0405 (4)
C20.45149 (16)0.63750 (14)0.69364 (15)0.0345 (4)
N30.42905 (13)0.59910 (12)0.79699 (12)0.0368 (4)
C40.5131 (2)0.51928 (18)0.84006 (18)0.0470 (5)
H410.560 (2)0.547 (2)0.910 (2)0.070*
H420.473 (2)0.454 (2)0.860 (2)0.070*
C50.5851 (2)0.50339 (18)0.73916 (18)0.0472 (5)
H510.670 (3)0.511 (2)0.762 (2)0.071*
H520.567 (2)0.430 (2)0.703 (2)0.071*
N60.39106 (13)0.71171 (12)0.63876 (12)0.0362 (4)
C70.30136 (15)0.75057 (14)0.69309 (14)0.0329 (4)
C80.27243 (16)0.71925 (14)0.79896 (15)0.0349 (4)
C90.34131 (16)0.63956 (14)0.85735 (14)0.0346 (4)
O100.24079 (12)0.82712 (10)0.63775 (11)0.0402 (3)
H1010.268 (2)0.844 (2)0.576 (2)0.060*
O110.33241 (12)0.60419 (10)0.95466 (10)0.0423 (3)
C120.17750 (17)0.77055 (15)0.85764 (17)0.0390 (4)
H1210.213 (2)0.7977 (18)0.933 (2)0.059*
H1220.150 (2)0.832 (2)0.814 (2)0.059*
C210.59787 (16)0.60289 (15)0.55615 (15)0.0384 (4)
C220.67539 (19)0.52838 (18)0.52397 (19)0.0500 (5)
H2210.691 (2)0.465 (2)0.568 (2)0.075*
C230.7284 (2)0.53957 (19)0.4242 (2)0.0534 (6)
H2310.777 (3)0.490 (2)0.404 (2)0.080*
C240.70459 (18)0.62511 (18)0.35695 (18)0.0499 (5)
C250.6293 (2)0.7008 (2)0.3878 (2)0.0568 (6)
H2510.617 (3)0.764 (2)0.342 (2)0.085*
C260.5754 (2)0.69008 (19)0.48719 (19)0.0511 (5)
H2610.529 (2)0.742 (2)0.507 (2)0.077*
Cl270.77155 (6)0.63967 (6)0.23211 (5)0.0784 (2)
C310.07284 (16)0.70368 (15)0.87807 (16)0.0389 (4)
C32−0.00662 (18)0.73742 (19)0.95069 (17)0.0489 (5)
C33−0.1022 (2)0.6786 (3)0.9736 (2)0.0669 (7)
H331−0.152 (3)0.706 (3)1.024 (3)0.100*
C34−0.1203 (2)0.5828 (3)0.9241 (3)0.0747 (8)
H341−0.183 (3)0.540 (3)0.942 (3)0.112*
C35−0.0442 (2)0.5470 (2)0.8503 (3)0.0742 (8)
H351−0.054 (3)0.479 (3)0.814 (3)0.111*
C360.0516 (2)0.60699 (18)0.8281 (2)0.0541 (5)
H3610.103 (3)0.581 (2)0.779 (2)0.081*
Cl370.01144 (6)0.85933 (6)1.01526 (7)0.0825 (3)
U11U22U33U12U13U23
N10.0425 (8)0.0461 (9)0.0342 (8)0.0134 (7)0.0110 (7)0.0067 (7)
C20.0374 (9)0.0386 (9)0.0281 (8)0.0033 (8)0.0064 (7)0.0001 (7)
N30.0419 (8)0.0412 (8)0.0283 (7)0.0055 (7)0.0082 (6)0.0041 (6)
C40.0524 (12)0.0506 (12)0.0387 (10)0.0142 (10)0.0088 (9)0.0098 (10)
C50.0523 (12)0.0496 (12)0.0405 (11)0.0157 (10)0.0089 (9)0.0103 (9)
N60.0395 (8)0.0411 (8)0.0296 (7)0.0070 (7)0.0107 (6)0.0026 (6)
C70.0364 (9)0.0338 (9)0.0293 (8)0.0012 (7)0.0071 (7)0.0003 (7)
C80.0391 (9)0.0364 (9)0.0305 (9)0.0004 (8)0.0100 (7)0.0008 (8)
C90.0397 (9)0.0368 (9)0.0284 (9)−0.0036 (8)0.0082 (7)−0.0026 (7)
O100.0456 (7)0.0434 (7)0.0335 (7)0.0109 (6)0.0129 (6)0.0068 (6)
O110.0570 (8)0.0452 (7)0.0265 (6)0.0006 (6)0.0127 (6)0.0035 (6)
C120.0436 (10)0.0387 (10)0.0370 (10)0.0016 (8)0.0145 (8)−0.0005 (9)
C210.0363 (9)0.0467 (10)0.0334 (9)0.0055 (8)0.0092 (7)−0.0008 (8)
C220.0525 (12)0.0496 (12)0.0506 (12)0.0134 (10)0.0173 (10)0.0013 (10)
C230.0525 (12)0.0555 (13)0.0557 (13)0.0110 (11)0.0212 (10)−0.0078 (11)
C240.0458 (11)0.0655 (14)0.0408 (11)0.0029 (10)0.0162 (9)−0.0037 (10)
C250.0606 (14)0.0656 (14)0.0476 (12)0.0159 (12)0.0211 (10)0.0134 (11)
C260.0538 (12)0.0584 (13)0.0447 (11)0.0178 (11)0.0210 (9)0.0086 (10)
Cl270.0858 (5)0.1015 (5)0.0555 (4)0.0106 (4)0.0425 (3)0.0026 (3)
C310.0380 (9)0.0458 (10)0.0335 (9)0.0007 (8)0.0067 (7)0.0036 (8)
C320.0413 (10)0.0673 (14)0.0395 (10)0.0036 (10)0.0105 (8)0.0005 (10)
C330.0432 (12)0.104 (2)0.0555 (14)−0.0044 (13)0.0165 (10)0.0133 (15)
C340.0489 (13)0.092 (2)0.0832 (19)−0.0194 (14)0.0082 (13)0.0247 (17)
C350.0642 (16)0.0622 (15)0.094 (2)−0.0200 (13)−0.0012 (15)−0.0006 (15)
C360.0501 (12)0.0532 (13)0.0597 (14)−0.0049 (10)0.0091 (10)−0.0086 (11)
Cl370.0628 (4)0.0959 (5)0.0929 (5)0.0075 (3)0.0269 (3)−0.0442 (4)
N1—C21.360 (2)C21—C221.385 (3)
N1—C211.411 (2)C21—C261.388 (3)
N1—C51.473 (2)C22—C231.383 (3)
C2—N61.305 (2)C22—H2210.97 (3)
C2—N31.358 (2)C23—C241.362 (3)
N3—C91.391 (2)C23—H2310.90 (3)
N3—C41.458 (2)C24—C251.373 (3)
C4—C51.528 (3)C24—Cl271.735 (2)
C4—H410.99 (3)C25—C261.384 (3)
C4—H420.99 (3)C25—H2510.97 (3)
C5—H510.99 (3)C26—H2610.90 (3)
C5—H521.04 (3)C31—C361.382 (3)
N6—C71.361 (2)C31—C321.382 (3)
C7—O101.330 (2)C32—C331.381 (3)
C7—C81.379 (2)C32—Cl371.740 (2)
C8—C91.421 (3)C33—C341.364 (4)
C8—C121.501 (2)C33—H3310.93 (3)
C9—O111.242 (2)C34—C351.374 (4)
O10—H1010.85 (3)C34—H3410.95 (4)
C12—C311.514 (3)C35—C361.388 (3)
C12—H1211.00 (3)C35—H3510.97 (4)
C12—H1220.97 (3)C36—H3610.93 (3)
C2—N1—C21127.93 (15)H121—C12—H122105.4 (19)
C2—N1—C5110.25 (15)C22—C21—C26118.77 (18)
C21—N1—C5121.37 (15)C22—C21—N1118.71 (18)
N6—C2—N3124.25 (16)C26—C21—N1122.50 (17)
N6—C2—N1126.25 (16)C23—C22—C21120.8 (2)
N3—C2—N1109.48 (15)C23—C22—H221117.5 (16)
C2—N3—C9122.42 (15)C21—C22—H221121.6 (16)
C2—N3—C4112.43 (15)C24—C23—C22119.7 (2)
C9—N3—C4124.92 (15)C24—C23—H231120.6 (19)
N3—C4—C5102.55 (15)C22—C23—H231119.7 (19)
N3—C4—H41108.5 (15)C23—C24—C25120.6 (2)
C5—C4—H41113.2 (15)C23—C24—Cl27119.78 (17)
N3—C4—H42111.4 (15)C25—C24—Cl27119.62 (18)
C5—C4—H42112.2 (15)C24—C25—C26120.2 (2)
H41—C4—H42109 (2)C24—C25—H251120.1 (17)
N1—C5—C4104.26 (16)C26—C25—H251119.6 (17)
N1—C5—H51108.7 (16)C25—C26—C21120.0 (2)
C4—C5—H51112.1 (16)C25—C26—H261118.3 (18)
N1—C5—H52111.8 (14)C21—C26—H261121.7 (18)
C4—C5—H52109.6 (14)C36—C31—C32116.41 (19)
H51—C5—H52110 (2)C36—C31—C12123.18 (17)
C2—N6—C7115.03 (15)C32—C31—C12120.40 (18)
O10—C7—N6114.97 (15)C33—C32—C31122.6 (2)
O10—C7—C8119.37 (16)C33—C32—Cl37117.77 (19)
N6—C7—C8125.63 (16)C31—C32—Cl37119.65 (16)
C7—C8—C9117.90 (16)C34—C33—C32119.8 (2)
C7—C8—C12122.85 (17)C34—C33—H331122 (2)
C9—C8—C12119.12 (15)C32—C33—H331118 (2)
O11—C9—N3117.86 (16)C33—C34—C35119.5 (2)
O11—C9—C8127.47 (16)C33—C34—H341121 (2)
N3—C9—C8114.66 (15)C35—C34—H341120 (2)
C7—O10—H101113.1 (17)C34—C35—C36120.1 (3)
C8—C12—C31116.73 (16)C34—C35—H351122 (2)
C8—C12—H121108.5 (14)C36—C35—H351118 (2)
C31—C12—H121107.9 (14)C31—C36—C35121.7 (2)
C8—C12—H122109.0 (14)C31—C36—H361119.5 (19)
C31—C12—H122108.6 (14)C35—C36—H361118.8 (19)
C21—N1—C2—N6−3.2 (3)C7—C8—C12—C31116.6 (2)
C5—N1—C2—N6−175.39 (19)C9—C8—C12—C31−67.8 (2)
C21—N1—C2—N3178.28 (17)C2—N1—C21—C22−164.0 (2)
C5—N1—C2—N36.0 (2)C5—N1—C21—C227.5 (3)
N6—C2—N3—C9−3.1 (3)C2—N1—C21—C2617.6 (3)
N1—C2—N3—C9175.46 (16)C5—N1—C21—C26−171.0 (2)
N6—C2—N3—C4−177.88 (19)C26—C21—C22—C23−0.9 (3)
N1—C2—N3—C40.7 (2)N1—C21—C22—C23−179.4 (2)
C2—N3—C4—C5−6.7 (2)C21—C22—C23—C240.3 (4)
C9—N3—C4—C5178.73 (18)C22—C23—C24—C250.6 (4)
C2—N1—C5—C4−9.9 (2)C22—C23—C24—Cl27179.68 (18)
C21—N1—C5—C4177.28 (18)C23—C24—C25—C26−0.9 (4)
N3—C4—C5—N19.5 (2)Cl27—C24—C25—C26180.0 (2)
N3—C2—N6—C70.4 (3)C24—C25—C26—C210.4 (4)
N1—C2—N6—C7−177.92 (18)C22—C21—C26—C250.6 (3)
C2—N6—C7—O10179.17 (15)N1—C21—C26—C25179.0 (2)
C2—N6—C7—C81.1 (3)C8—C12—C31—C36−12.0 (3)
O10—C7—C8—C9−178.03 (16)C8—C12—C31—C32167.16 (18)
N6—C7—C8—C9−0.1 (3)C36—C31—C32—C330.3 (3)
O10—C7—C8—C12−2.3 (3)C12—C31—C32—C33−178.9 (2)
N6—C7—C8—C12175.65 (17)C36—C31—C32—Cl37−178.73 (17)
C2—N3—C9—O11−175.20 (17)C12—C31—C32—Cl372.1 (3)
C4—N3—C9—O11−1.1 (3)C31—C32—C33—C340.4 (4)
C2—N3—C9—C83.9 (2)Cl37—C32—C33—C34179.5 (2)
C4—N3—C9—C8178.01 (19)C32—C33—C34—C35−1.2 (4)
C7—C8—C9—O11176.67 (18)C33—C34—C35—C361.2 (4)
C12—C8—C9—O110.8 (3)C32—C31—C36—C35−0.3 (3)
C7—C8—C9—N3−2.4 (2)C12—C31—C36—C35178.9 (2)
C12—C8—C9—N3−178.25 (16)C34—C35—C36—C31−0.5 (4)
D—H···AD—HH···AD···AD—H···A
C12—H122···O100.97 (2)2.41 (2)2.848 (2)106.5 (17)
C26—H261···N60.90 (2)2.36 (2)2.918 (3)120.3 (19)
O10—H101···O11i0.85 (2)1.80 (2)2.6418 (18)172 (3)
C33—H331···Cl27ii0.93 (4)2.81 (4)3.534 (2)135 (3)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C12—H122⋯O100.97 (2)2.41 (2)2.848 (2)106.5 (17)
C26—H261⋯N60.90 (2)2.36 (2)2.918 (3)120.3 (19)
O10—H101⋯O11i0.85 (2)1.80 (2)2.6418 (18)172 (3)
C33—H331⋯Cl27ii0.93 (4)2.81 (4)3.534 (2)135 (3)

Symmetry codes: (i) ; (ii) .

  5 in total

1.  The Cambridge Structural Database: a quarter of a million crystal structures and rising.

Authors:  Frank H Allen
Journal:  Acta Crystallogr B       Date:  2002-05-29

2.  New software for searching the Cambridge Structural Database and visualizing crystal structures.

Authors:  Ian J Bruno; Jason C Cole; Paul R Edgington; Magnus Kessler; Clare F Macrae; Patrick McCabe; Jonathan Pearson; Robin Taylor
Journal:  Acta Crystallogr B       Date:  2002-05-29

3.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

4.  Synthesis and pharmacological activity of new carbonyl derivatives of 1-aryl-2-iminoimidazolidine. Part 3. Synthesis and pharmacological activity of 1-aryl-5,6(1H)dioxo-2,3-dihydroimidazo[1,2-a]imidazoles.

Authors:  Dariusz Matosiuk; Sylwia Fidecka; Lucyna Antkiewicz-Michaluk; Izabela Dybala; Anna E Koziol
Journal:  Eur J Med Chem       Date:  2002-10       Impact factor: 6.514

5.  Synthesis and pharmacological activity of new carbonyl derivatives of 1-aryl-2-iminoimidazolidine: part 2. Synthesis and pharmacological activity of 1,6-diaryl-5,7(1H)dioxo-2,3-dihydroimidazo[1,2-a][1,3,5]triazines.

Authors:  Dariusz Matosiuk; Sylwia Fidecka; Lucyna Antkiewicz-Michaluk; Janusz Lipkowski; Izabela Dybala; Anna E Koziol
Journal:  Eur J Med Chem       Date:  2002-09       Impact factor: 6.514

  5 in total

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