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. Author manuscript; available in PMC: 2013 Oct 15.
Published in final edited form as: Inorg Chem. 2012 Sep 27;51(20):10619–10630. doi: 10.1021/ic300852t

Cadmium(II) Complex Formation with Selenourea and Thiourea in Solution: An XAS and 113Cd NMR Study

Farideh Jalilehvand 1,*, Zahra Amini 1, Karnjit Parmar 1
PMCID: PMC3498765  NIHMSID: NIHMS411111  PMID: 23016594

Abstract

The complexes formed in methanol solutions of Cd(CF3SO3)2 with selenourea (SeU) or thiourea (TU), for thiourea also in aqueous solution, were studied by combining 113Cd NMR and X-ray absorption spectroscopy. At low temperature (~200 K) distinct 113Cd NMR signals were observed, corresponding to CdLn2+ species (n = 0 - 4, L = TU or SeU) in slow ligand exchange. Peak integrals were used to obtain the speciation in the methanol solutions, allowing stability constants to be estimated. For cadmium(II) complexes with thione (C=S) or selone (C=Se) groups coordinated in Cd(S/Se)O5 or Cd(S/Se)2O4 (O from MeOH or CF3SO3-) environments the 113Cd chemical shifts were quite similar, within 93-97 ppm and 189 – 193 ppm, respectively. However, the difference in the chemical shift for the Cd(SeU)42+ (578 pm) and Cd(TU)42+ (526 ppm) species, with CdSe4 and CdS4 coordination, respectively, shows less chemical shielding for the coordinated Se atoms than for S, in contrast to the common trend with increasing shielding in the order: O > N > Se >S. In solutions dominated by mono- and tetra-thiourea / selenourea complexes, their coordination and bond distances could be evaluated by Cd K-edge extended X-ray absorption fine structure (EXAFS) spectroscopy. At ~200 K and high excess of thiourea a minor amount (up to ~30%) of [Cd(TU)5-6]2+ species was detected by an upfield shift of the 113Cd NMR signal (up to 423 ppm) and an amplitude reduction of the EXAFS oscillation. The amount was estimated by fitting linear combinations of simulated EXAFS spectra for [Cd(TU)4]2+ and [Cd(TU)6]2+ complexes. At room temperature, [Cd(TU)4]2+ was the highest complex formed, also in aqueous solution. Cd L3-edge X-ray absorption near edge structure (XANES) spectra of cadmium(II) thiourea solutions in methanol were used to follow changes in the CdSxOy coordination at room temperature. The correlations found from the current and previous studies between 113Cd NMR chemical shifts and different Cd(II) coordination environments are generally useful for evaluating cadmium coordination to thione-containing or Se-donor ligands in biochemical systems or for monitoring speciation in solution.

Keywords: Cadmium(II), selenourea, thiourea, Cd K-edge EXAFS, Cd L3-edge XANES, 113Cd NMR

Introduction

Thione-containing molecules have important biochemical functions and also industrial applications. For example, L-ergothioneine (a thiohistidine) is a naturally occurring amino acid with antioxidant properties that can be made by few organisms (bacteria and fungi), taken up by plants and ingested by animals and human.1 It has two tautomeric forms: thiol and thione;2 the latter predominates at physiological pH in aqueous solution,3 and can form complexes with many metal ions: Cu(II) > Hg(II) > Zn(II) > Cd(II) > Ni(II) ~ Co(II), in order of increasing stability.4,5 Some diabetic patients obtain high levels of ergothioneine, which due to the high stability of its zinc complexes (logβ2 ~1012),4 leads to zinc deficiency and glucose intolerance.6 Also, it has been shown that ergothioneine has protective effects toward cadmium-induced teratogenesis.7

Increasing our knowledge about how interactions related to group 12 zinc(II) and cadmium(II) ions affect biological systems is essential. Although its ionic radius is larger (~0.2 Å),8 cadmium(II) is known to attach to the binding sites of Zn-enzymes / proteins with higher affinity than zinc(II) and thereby inhibit important functions.9,10 Thiourea (TU, Scheme 1) provides a structurally simple model for studies of thione-containing ligands. The structures of many metal-thiourea complexes, in which the thiourea molecule is coordinated to the metal center via its S atom, are available in the Cambridge structural database (CSD),11 as e.g. for the four-coordinated [Cd(TU)2Cl2],12 [Cd(TU)4](NO3)2,13 and six-coordinated [Cd(TU)2(NO3)2],13 [Cd(TU)2(HCOO)2],14 and [Cd(TU)6](ReO4)2 complexes.15 In aqueous solution cadmium(II) complexes with up to four thiourea ligands have been reported with the formation constants β1 = 20, β2 = 140, β3 = 260 and β4 = 1200 (Figure S-1), based on a polarographic study.16

Scheme 1.

Scheme 1

Thiourea (TU) and selenourea (SeU)

CdS semiconducting nanoparticles (NPs) and thin films have promising photo-electrochemical applications, e.g. in solar cells.17 Highly luminescent water-soluble CdS NPs can be prepared by thermal decomposition of Cd(II) and thiourea mixtures. Their size influences the optical activity,18 and the photoluminescence quantum yield depends on pH, and the concentration and ratio of thiourea to cadmium(II).19,20 O’Brien and Saeed deposited thin films of CdS from alkaline solutions of Cd(CH3COO)2, ethylenediamine and thiourea, and correlated the quality and morphology of CdS thin films to the conditions used for growth, e.g. by following speciation changes in the solution by 113Cd NMR spectroscopy.21 The observed 113Cd NMR chemical shifts, however, were not connected to specific Cd(II) species. 113Cd NMR spectroscopy has also been used to investigate the formation mechanism of Cd NPs through oxidative aggregation of [Cd10S4Br4(SR)12]4- (SR = p-tolylthiolate) by elemental sulfur.22

CdSe NPs and thin films have been prepared from mixtures of selenourea and cadmium salts in similar ways as for cadmium sulfide. Selenourea (SeU, Scheme 1) is a resonance-stabilized selenoketone (selone) with π-conjugation between the selenocarbonyl and amino groups.23 It is sensitive to heat, light and moisture and is easily oxidized in acidic aqueous solution forming a Se-Se bond in a diselenobis(formamidinium) cation,24 or decomposed by atmospheric oxygen to red elemental selenium in neutral / alkaline aqueous solution,25 and even in methanol and ethanol.26 Hydrolytic decomposition of selenourea generates cyanamide (H2CN2), Se2- and HSe-, and is accelerated by increasing pH.25,27,28 Hydrochemical decomposition of metal selenourea compounds to metal selenide nanoparticles is a common procedure for generating thin films for new semiconductor materials.27

While several reports on syntheses of simple selenourea metal complexes all conclude that the Se atom is the only coordination site for metal ions,26,29,31 very few crystal structures are available32,33 (apart from a few with selenourea derivatives). There is only one structurally known complex where a selenourea derivative, N,N’-diphenylselenourea, acts as a bidentate ligand with (Se, N) coordination to a Pt(II) ion.34 A series of selenourea complexes with different Co(II), Zn(II), Cd(II) and Hg(II) salts including Cd(SeU)2X2 (X = halide), were prepared and carefully analyzed using electronic (UV-vis.) and vibrational (IR) spectroscopic techniques, reporting metal-selenium stretching vibrations within the range 167 – 245 cm-1.35 A solid state 113Cd NMR spectrum of [Cd(SeU)2Cl2] showed an isotropic chemical shift of δiso(113Cd) = 458 ppm.36 Recently, spray hydrolysis of [Cd(SeU)2Cl2] in aqueous solution, prepared by reacting CdCl2 hydrate with 4-fold selenourea, was used to generate CdSe films.37 CdSe nanocrystals have also been prepared by fast injection of a base to a solution of Cd(NO3)2·4H2O and selenourea at room temperature. The mechanism of this reaction seems to be via an unidentified intermediate Cd-selenourea complex.38 A polarographic study showed that Cd(II) ions form a selenourea complex with limited solubility in de-aerated water with [Cd2+] = 0.01 mM.39 The formation constant for the 1:1 complex between cadmium(II) and SeU was recently determined to be log β1 = 2.11 ± 0.04 in 0.5 mol dm-3 HClO4 and ionic strength I = 1.0 (NaClO4) at 298 K using UV-vis. spectroscopy,40 which differs from the previously reported value log β1 = 0.9 (log β2 = 3.7) using a cadmium amalgam electrode.41

In the current study, we compared the complex formation of cadmium(II) ions with selenourea and thiourea as ligands, keeping CCd(II) = 0.1 mol dm-3 and varying the mole ratios SeU / Cd(II) from 1.0 to 5.0 and TU / Cd(II) from 1.0 to 20.0. The speciation and structure of the complexes were investigated with 113Cd NMR spectroscopy as the main tool, complemented by Cd K-edge EXAFS and Cd L3-edge XANES spectra. Methanol was chosen as solvent because selenourea reacts with water,25 and it also allowed low temperature studies (at ~200 K). In addition, the cadmium(II)- thiourea complexes formed in aqueous solution were studied at room temperature.

113Cd NMR spectroscopy has in the past few decades developed into a powerful tool for studying the coordination of cadmium ions in compounds and biological systems.42,43 The 113Cd NMR chemical shift depends on several factors including: number and type of the donor atoms (with the general trend O > N > Se > S, in order of increasing shielding) and the coordination geometry around cadmium, the nature and charge of the ligand (e.g. different shielding of sulfur in thiolate S- and thiocyanate SCN-) and its coordination mode (bridging vs. terminal).43,44 This is evident from the 113Cd NMR isotropic chemical shifts (δiso) for crystalline Cd(II) complexes with S-thione containing ligands in Table 1, and the 113Cd NMR chemical shifts for Cd(II) complexes with Se-donor ligands in Table 2. In solution ligand-exchange dynamics affects the peak shape and peak position, which becomes a weighted average of the chemical shifts of all Cd(II) species involved in fast ligand-exchange equilibria.45 The temperature and the nature of the solvent also influence the 113Cd NMR chemical shift.

Table 1.

Solid state 113Cd NMR isotropic chemical shifts (δiso) for crystalline Cd(II) complexes with S-thione containing ligands; see Figures S-3 and S-4 (a, b)

Cd(II)-thione compounds a Coordination 113Cd NMR chemical shift (δiso, ppm) Reference
[Cd(tztH)4](CF3SO3)2 CdS4 605 b 46
[Cd(TU)4](NO3)2 CdS4 577 (this work) 13
[Cd(TU)2Cl2] CdS2Cl2 462 c 36
[Cd(tzt)2] CdS2N2 430 b 47
[Cd(DMTF)6](ClO4)2 CdS6 402 (this work) 48
(HIm)[Cd(tsac)3(H2O)] CdS3O 378 (this work) 49
[Cd(TU)3(SO4)] CdS3O 346 (this work) 50
[Cd2(6-MP)4(H2O)2](NO3)4 CdS3N2O 313 51
trans-[Cd(DMTF)4(CF3SO3)2] CdS4O2 263 (this work) 48
[Cd2(6-MP)4(NO3)2](NO3)2 CdS3N2O2 233 51
cis-[Cd(TU)2(H2O)4](SO4) CdS2O4 148 (this work) 52
a

tztH = 1,3-thiazolidine-2-thione, DMTF = dimethylthioformamide, HIm = imidazolium, tsac = thiosaccharinato (with negatively charged thionate-S)49, 6-MP = 6-mercaptopurine;

b

the calibration is shifted (see the text) by changing δiso for the solid reference compound 3CdSO4·8H2O from -77.4 to -58 ppm;

c

the calibration is shifted by changing δiso for the solid reference compound Cd(NO3)2·4H2O from -132.2 to -100 ppm.

Table 2.

113Cd NMR chemical shifts for mononuclear Cd(II) complexes with Se-donor ligands

Cd(II) compounds a Coordination 113Cd NMR chemical shift (δ, ppm) Reference
[Cd(dmpSe)2](ClO4)2 CdSe2P2 670 (CH2Cl2, 193 K) 55
Cd[N(iPr2PSe)2]2 CdSe4 629 (solid) 56
CdSe (bulk) CdSe4 558 (solid) b 57,58
[Cd(SePh)4](NO3)2 CdSe4 533 (CH3OH, 213 K) c 59
Cd(L-ImSe)2Cl2 CdSe2Cl2 506 – 591 (solid) d 60
Cd(SeU)2Cl2 CdSe2Cl2 490 (solid) d 36
[Cd(Se-aryl)2(bpy)] CdSe2N2 460, 472 (solid), 411 (CHCl3) 61
[Cd(SeC(O)R’)2(tmeda)] CdSe2N2O2 388 - 391 (CDCl3) e 62
[Cd(SeC5H4N)2(tmeda)] CdSe2N4 300 (CDCl3) e 63
(Ph4P)[Cd(SeC(O)Tol)3] CdSe3O2 250 (CH2Cl2, 193 K) 64
a

dmpSe = Ph2PCH2P(Se)Ph2; N(iPr2PSe)2- = Tetraisopropyldiselenoimidodiphosphoinato; -SePh = phenylselenolate; L-ImSe = imidazolidine-2-selone, L = H, CH3, C2H5, n-C3H7, i-C3H7; Se-aryl = -Se-2,4,6-iPr3-C6H2; R’ = Ph, Tol, Tol = C6H4-p-CH3; tmeda = N,N,N’,N’-tetramethylethylenediamine;

b

The value reported here is referenced relative to Cd(ClO4)2 (aq) by changing the chemical shift of solid Cd(NO3)2·4H2O from 0.0 to -100 ppm43;

c

the calibration for 4.5 mol·dm-3 Cd(NO3)2 (aq) was changed from -65 to -73 ppm;

d

the calibration was adjusted by changing δiso for Cd(NO3)2.4H2O from -132.2 to - 100 ppm;

e

reported relative to Cd(CH3COO)2·2H2O in CH3OD (0.0 ppm).

113Cd NMR chemical shifts from different sources are sometimes calibrated with different standards.53 To keep consistency in Tables 1 and 2 between our 113Cd chemical shifts calibrated as 0 ppm for solid Cd(ClO4)2·6H2O and those previously reported, we have used -100 ppm as calibration point for solid Cd(NO3)2·4H2O, and -45 and -58 ppm for the two signals for solid 3CdSO4·8H2O.54 For the solution spectra our calibration 0 ppm for 0.1 mol·dm-3 Cd(ClO4)2(aq) corresponds to -73 ppm for 4.5 mol·dm-3 Cd(NO3)2(aq) (Table 2).43

The low temperature measurements presented here show that at ~200 K the Cd(II)-selenourea and most Cd(II)-thiourea complexes are in slow ligand-exchange, resulting in a separate 113Cd NMR peak for each Cd(II) complex (Figure 1). Their peak positions and areas allowed quantitative speciation of the Cd(II)-thione / selone complexes, and also an estimate of their stability constants. The EXAFS studies of the solutions with a dominating Cd(II)-thione / selone complex corroborated the assignments of the 113Cd NMR resonances and provided additional structural information.

Figure 1.

Figure 1

113Cd NMR spectra of 0.1 mol dm-3 Cd(CF3SO3)2 methanol solutions with increasing mole ratios L/Cd(II) of selenourea (S1 – S5; left, at 203 K) or thiourea (T1 – T7; middle at 203 K; right at 295 K). For notations see Table 3.

The results and the methodology used in this research provide benchmarks for evaluating coordination environments involving Cd(II) ions and thione/ selone groups in complex biological systems, or for monitoring speciation in solution, e.g. to control the formation of CdS/ CdSe nanoparticles via thiourea/ selenourea complexes.

Experimental Section

Sample preparation

Selenourea, thiourea and methanol-d4 (CD3OD) from Sigma-Aldrich were used without further purification. Methanol (MeOH) was dried by refluxing twice over magnesium turnings under argon atmosphere. Dehydrated cadmium triflate Cd(CF3SO3)2 was prepared by dissolving freshly prepared Cd(OH)2 in triflic acid, in a procedure described previously.65

Cadmium(II) selenourea / thiourea solutions

Cadmium(II) triflate solutions with [Cd2+]tot = 0.1 mol dm-3 and varying amounts of SeU or TU in O2-free, dried methanol were prepared in a glove box with dry inert atmosphere. For the 113Cd NMR measurements the solvent contained 30% CD3OD. Five solutions with SeU / Cd(II) mole ratios of 1.0 (S1), 2.0 (S2), 3.0 (S3), 4.0 (S4) and 5.0 (S5) were prepared. Higher SeU / Cd(II) mole ratios were prevented by the limited solubility of SeU in methanol at ~200 K. Similar cadmium(II) thiourea solutions in methanol were prepared with TU / Cd(II) mole ratios 1.0 (T1), 2.0 (T2), 3.0 (T3), 4.0 (T4), 5.0 (T5), 8.0 (T6) and 10.0 (T7). To check the solvent effect, a parallel series of Cd(II)-thiourea solutions (W1 to W9) were prepared in distilled water containing 10% D2O. Table 3 presents the composition of the solutions.

Table 3.

Composition of the cadmium(II)-selenourea and thiourea solutions a

Solutions in MeOH L/CdII mole ratio [Cd2+]total (mmol·dm-3) [L]total (mmol·dm-3) Solutions in H2O
L = SeU
S1 1.0 100 100
S2 2.0 100 200
S3 3.0 100 300
S4 4.0 100 400
S5 5.0 100 500
L = TU
T1 1.0 100 100 W1
T2 2.0 100 200 W2
T3 3.0 100 300 W3
T4 4.0 100 400 W4
T5 5.0 100 500 W5
T6 8.0 100 800 W6
T7 10.0 100 1000 W7
100 1500 W8
100 2000 W9
a

For 113Cd NMR measurements, the methanol solutions contained 30% CD3OD and aqueous solutions 10% D2O.

113Cd NMR reference compounds

The crystalline cadmium(II) dimethylthioformamide (DMTF) compounds [Cd(DMTF)6](ClO4)2 (coordination model for CdS6) and [Cd(DMTF)4(CF3SO3)2] (CdS4O2 model), imidazolium tris(thiosaccharinato)aquacadmate(II) (HIm)[Cd(tsac)3(H2O)] (CdS3O model), and [Cd(TU)4](NO3)2 (CdS4 model) were synthesized according to descriptions in the literature,13,48,49 and were verified by comparing their unit cell dimensions with those of the known structures (Figure S-2).

113Cd NMR measurements

The 113Cd NMR spectra of the methanol solutions S1-S5 and T1-T7 were collected at 203 K with a Bruker DRX-400 spectrometer at 88.56 MHz, using a 5 mm broadband (BBO) probe, zgdc pulse program, a sweep width of 800 ppm, and recycle delay of 3.0 seconds. All the above solutions contained ~ 30% CD3OD. A 0.1 mol·dm-3 solution of Cd(ClO4)2·6H2O in D2O was used as external reference (0 ppm at 295 K).43 The temperature of the instrument was calibrated using 1H NMR of methanol.66 The spectra of the Cd(II)-thiourea solutions T1 – T7 in methanol and W1 – W9 in water (10% D2O) were also measured under similar conditions at room temperature (295 K). The total number of scans collected for each sample can be found in Table S-1a. The integrated areas of the peaks in the 113Cd NMR spectra of the methanol solutions T1 – T3 and S1 – S3 (203 K) are listed in Table S-1b.

Solid state 113Cd NMR spectra of the crystalline cadmium(II) reference compounds were measured using a Bruker AMX 300 spectrometer equipped with a MAS BL4 double-resonance broadband probe, at the resonance frequency 66.59 MHz. The samples were packed into 4 mm ZrO rotors with magic angle spinning (MAS) rates between 5 – 8 kHz. Solid Cd(ClO4)2·6H2O was used for calibration (0 ppm at room temperature). Spectra were acquired at 300 K using a 4 μs 1H 90° pulse, 4 ms contact time and 10 s recycle delay. The isotropic chemical shifts are listed in Table 1.

X-ray absorption spectroscopy

Cadmium K-edge EXAFS spectra of the solutions S1, S5, T1 - T7 were collected at BL 7-3, and Cd L3-edge XANES spectra of solutions T1 – T7 were measured at room temperature at BL 4-3 at the Stanford Synchrotron Radiation Lightsource (SSRL) with the storage ring operated at 3.0 GeV and 150-200 mA. The EXAFS spectra for solutions S1 and S5 were measured at 200 K (LT) by means of a liquid-helium cryostat, while for T1 – T7 spectra were collected both at 200 K and at room temperature (RT). Pure methanol solidifies below ~ 179 K, so by keeping the temperature at 200 K the samples remained unfrozen and were kept inside the cryostat under chilled air flow (not vacuum) at all times (Note: N2 in the air freezes below ~ 80 K). At BL 7-3, higher harmonics from the Si(220) double crystal monochromator were rejected by detuning to 50% of the maximum incident beam (I0) intensity, while a Rh-coated mirror was used at BL 4-3 to eliminate higher harmonics from a fully tuned Si(111) double crystal monochromator. The EXAFS spectra were recorded in transmission mode, with all ion chambers filled with argon, while the Cd L3-edge XANES spectra were measured in fluorescence mode using a PIPS solid state detector (If) and a helium-filled ion chamber (I0) monitoring the X-ray fluorescence and incident beam intensities, respectively. For EXAFS measurements, the samples were held between Kapton windows in 2 mm pinhole cells sealed with vacuum grease at LT, or in 5 mm Teflon spacers at RT. Two to six scans (10 for S1) were collected for each sample. During the Cd L3-edge XANES measurements, two scans were measured for each solution held within a 5 mm Teflon spacer between 4 μm Ultralene© windows that were found to resist penetration of He gas that otherwise could form bubbles in the sample. Before averaging the overlapping scans using the EXAFSPAK program,67 the energy scale was externally calibrated for each scan by assigning the first inflection point of the Cd K- and L3-edge of a Cd foil to 26711.0 eV and 3537.6 eV, respectively.

XAS data analysis

The WinXAS 3.1 program suite was used for the data analysis.68 The background absorption was subtracted with a first-order polynomial over the pre-edge region, followed by normalization of the edge step. For the Cd K-edge EXAFS spectra, the energy scale was converted into k-space, where k = [(8π2me/h2)(E-E0)]1/2, using the threshold energy E0 = 26709.7 – 26711.0 (S1, S5), 26710.0 – 26713.0 eV (T1 – T7 and W1 – W7). The EXAFS oscillation was then extracted using a 7-segment cubic spline to remove the atomic background absorption above the edge. Details on extraction of structural parameters from the experimental EXAFS oscillation can be found elsewhere.69 Theoretical EXAFS oscillations, χ(k), were constructed using the FEFF 8.1 program,70,71 with FEFF input files generated by means of the ATOMS program72 using the crystal structures of Cd(SCH2CH2NH2)2,73 [Cd(dmise)4][PF6]2 where dmise = 1,3-dimethyl-2(3H)-imidazoleselone,74 and [Cd(CH2(COO)2)(TU)2]75 (replacing S by Se in the input file), with CdS3N2, CdSe4 and CdS2O3 coordination geometries, respectively. Note that two neighboring elements in the periodic table (such as oxygen and nitrogen) with very similar amplitude functions cannot be distinguished by EXAFS.

The structural parameters were refined by least-squares methods, fitting the model function χ(k) to the experimental unfiltered EXAFS oscillation using k3-weighting, generally over the k range 3 – 14 Å-1, allowing the bond distance (R), Debye-Waller parameter (σ) and ΔE0 (with a common value for all scattering paths) to float, while the amplitude reduction factor (S02) and / or coordination number (N) were fixed. The S02 value refined to 0.99 at the EXAFS data analysis for crystalline [Cd(TU)4](NO3)2 with the coordination number fixed (4 Cd-S; Figure S-7). This parameter value was then kept fixed at 1.0 during the EXAFS curve-fitting process for the solutions (Tables 4, 5 and S-2). The accuracy of the refined coordination numbers N, bond distances R and their Debye-Waller parameters (σ2) for the dominating Cd-Se and Cd-S paths are estimated to be within ± 20%, ± 0.02 Å and ±0.001 Å2, respectively, accounting for effects of systematic deviations in the extracted data, model limitations, correlated parameters, etc. The above error limits were estimated from variations in the parameter values when refining models of different complexity, systematically varying the k-range, or when trying different cubic spline removals. The corresponding structural parameters for the Cd-O path are less accurate, ± 0.04 Å for bond distances (± 0.02 Å for SeU complexes) and ± 0.002 Å2 (± 0.001 Å2 at LT) for Debye-Waller parameters σ2, due to the difficulties associated with separating the EXAFS contribution from the oxygen (or nitrogen) atoms when their mean bond distance is rather close to that of the heavier sulfur atoms.

Table 4.

Structural Parameters Derived from EXAFS Least-Squares Curve Fitting for the Cd(II)-SeU Methanol Solutions S1 and S5 at 200 K (CCd(II) ~0.1 mol dm-3; see Figure 3). a

Solution (SeU/Cd(II) Cd-O Cd-Se

N R (Å) σ22) N R (Å) σ22) b
S1 (1.0) 5 f 2.29 0.0066 1 f 2.62 0.0036 18.0
S5 (5.0) 3.8 2.63 0.0043 24.4
a

Fitting k-range = 3 - 14 Å-1; S02 = 1.0 f (f = fixed); estimated error limits: N ± 20 %, R ± 0.02 Å, σ2 ± 0.001 Å2.

b
Residual; the residual (%) from the least-squares curve fitting is defined as:
i=1N|yexp(i)­ytheo(i)|i=1N|yexp(i)|×100
where yexp and ytheo are k3-weighted experimental and theoretical data points, respectively.

Table 5.

Structural Parameters Derived from EXAFS Least-Squares Curve Fitting of Models for the Cd(II)-TU Methanol Solutions T1, T2, T4 - T7 at 200 K (LT) and 298 K (RT); (CCd(II) ~0.1 mol dm-3; see Figure 4). a

Solution (TU / Cd(II) mole ratio) 113Cd δ (ppm) Cd-S Cd-O

N R (Å) σ22) N R (Å) σ22) b
[Cd(TU)4](NO3)2 solid 577 (δiso) 4 f 2.53 0.0063 15.4
Temp. 200 K
T1 (1.0) -21, 93 (major), 189 1 f 2.54 0.0030 5 f 2.30 0.0047 17.4
T2 (2.0) 94, 191 (major), 337 2 f 2.55 0.0056 4 f 2.33 0.0062 14.3
T4 (4.0) 515 (broad) 3.8 2.53 0.0052 13.9
T5 (5.0) 506 3.8 2.54 0.0057 13.4
T6 (8.0) 458 3.3 2.54 0.0066 22.2
T7 (10.0) 423 3.8 2.55 0.0087 20.6
Temp. 298 K
T1 (1.0) 1 f 2.54 0.0063 5 f 2.30 0.0075 14.2
T2 (2.0) 2 f 2.51 0.0066 4 f 2.34 0.0132 18.2
T4 (4.0) 503 3.3 2.52 0.0060 8.1
T5 (5.0) 534 3.3 2.53 0.0057 10.7
T6 (8.0) 541 3.3 2.53 0.0053 13.9
T7 (10.0) 533 3.5 2.53 0.0063 10.1
a

k-range for fitting 3 - 14 Å-1; S02 = 1.0 f (f = fixed) for solutions; estimated error limits: N ± 20 %, for Cd-S R ± 0.02 Å, σ2 ± 0.001 Å2; for Cd-O R ± 0.04 Å and σ2 ± 0.002 Å2;

b

residual.

To the experimental LT EXAFS spectra of solutions T6 and T7 linear combinations of simulated EXAFS oscillations for CdS4 and CdS6 coordination were fitted in the k range 3.4 – 14.4 Å-1, following a procedure explained elsewhere,76 with the S02 and ΔE0 values fixed at 1.0 and 1.0 eV, respectively. The simulations were performed for CdS4 by varying the average Cd-S distance in the range 2.53 – 2.54 Å (σ2 = 0.005 – 0.007 Å2) and for CdS6 2.68 – 2.74 Å (σ2 = 0.006 – 0.007 Å2). The best fits were obtained with the following parameters: CdS4 (4 Cd-S, R = 2.54 Å, σ2 = 0.005 Å2) and CdS6 (6 Cd-S, R = 2.71 Å, σ2 = 0.007 Å2).

Results

113Cd NMR spectroscopy

113Cd NMR spectra were measured at 203 K of 0.1 mol dm-3 dehydrated Cd(CF3SO3)2 in methanol solutions (30% CD3OD) containing different concentrations of thiourea (T1 – T7) or selenourea (S1 – S5) (see Figure 1 left and middle). The spectrum of Cd(CF3SO3)2 in methanol without added ligands (L = TU, SeU) showed a signal at -21 ppm. In the solutions S1 and T1, both with the mole ratio L/Cd(II) = 1.0, several sharp signals with similar 113Cd chemical shifts appeared. A small peak at -21 ppm showed that at this mole ratio some Cd(II) ions still remained free, however, at increasing ligand concentration this signal disappeared. For the methanol solutions S2 – S3 and T2 – T3 with L/Cd(II) mole ratios 2.0 and 3.0 (L = TU, SeU), respectively, up to five distinct 113Cd NMR signals appeared indicating four Cd(II) species with different coordination environments in slow ligand-exchange equilibria, beside the solvated Cd2+ ion.

The first two sharp signals appeared with very similar chemical shifts: 94 and 191 ppm for T2 and T3, versus 97 and 194 ppm for S2 and S3, while the next two signals were broader and more shielded for the Cd(II)-thiourea solutions T2 and T3 (333 and 526 ppm) than for the Cd(II)-selenourea solutions S2 and S3 (435 and 578 ppm). For solutions S4 and S5 only one single sharp signal at 578 ppm remained, corresponding to a single dominating Cd(II)-selenourea complex. Also the Cd(II) thiourea solutions T4 to T7 displayed a single, relatively broad peak. However, the gradual increase in shielding from 515 ppm in T4 to 423 ppm in T7 with increasing thiourea concentration can be attributed to a gradual change in the coordination environment around Cd(II).

The 113Cd NMR spectra obtained for the thiourea solutions T4 – T7 at room temperature are shown in Figure 1 (right). No signal could be obtained for T1 – T3, since the 113Cd NMR signals became broader and finally disappeared at 223 K. For solutions T4 – T7 the single 113Cd NMR signal became considerably sharper and mostly less shielded at RT, which means that either a single dominating Cd(II) thiourea complex is present, or that the Cd(II)-thiourea species are in fast ligand exchange.

To investigate the influence of the solvent on the Cd(II)- thiourea complex formation, 113Cd NMR spectra were measured of a series of aqueous 0.1 mol dm-3 Cd(CF3SO3)2 solutions with different TU / Cd(II) mole ratios (Figure 2). All spectra showed a single sharp signal, which with increasing ligand concentration gradually became less shielded, from δ(113Cd) = 1 ppm for 0.1 mol dm-3 Cd(CF3SO3)2 in aqueous solution, 60 ppm with 0.1 mol dm-3 thiourea in W1, to 446 ppm for 2.0 mol dm-3 thiourea in W9 (mole ratio TU / Cd(II) = 20), indicating that S ligand atoms gradually replace O atoms in the Cd(II) coordination environment.

Figure 2.

Figure 2

113Cd NMR spectra of 0.1 mol dm-3 Cd(CF3SO3)2 aqueous solutions (W1 – W9) with thiourea mole ratios TU / Cd(II) increasing from 1.0 to 20.0, measured at 295 K; see Table 3. The spectrum at the top is for a solution without added thiourea.

X-ray absorption spectroscopy - Cd K-edge EXAFS

Cd K-edge EXAFS spectra were measured at 200 K for the methanol solutions S1 and S5 with the SeU / Cd(II) mole ratios 1.0 and 5.0, respectively (Figure 3); the curve-fitting results are shown in Table 4. Solutions S2, S3 and S4 were not measured, since the 113Cd NMR measurements showed that solutions S2 - S3 contained mixtures of Cd(II)-SeU complexes and that the speciation was similar in solution S4 as in S5. Also solution S1 contained several Cd(II)-SeU complexes, with the dominating one giving a signal at δ(113Cd) = 96 ppm (Figure 1, left). The EXAFS oscillation of this solution was well fitted with a model containing one SeU ligand and five oxygen donors from solvent (methanol) molecules and possibly also the CF3SO3- anion, with average Cd-Se and Cd-O bond distances of 2.62 ± 0.02 Å and 2.29 ± 0.02 Å, respectively. This model is supported by a calculation of the average number of bound SeU per Cd(II) ion (= 1.01) from the 113Cd NMR peak integrals, which correspond to the fraction of each Cd(II) complex in solution S1 (Appendix 1, Supporting Information). The EXAFS oscillation of solution S5 with considerably higher amplitude than that of S1 was well modeled by four Cd-Se paths at 2.63 ± 0.02 Å (Table 4).

Figure 3.

Figure 3

Cd K-edge EXAFS curve-fitting for the Cd(II)-selenourea methanol solutions S1 and S5 with SeU/ Cd(II) mole ratios 1.0 and 5.0 (CCd(II) = 0.1 mol dm-3 measured at 200 K (see Table 4)

For the series of Cd(II) thiourea solutions T1 – T7 (excluding T3) in MeOH, Cd K-edge EXAFS spectra were measured at both 200 K (LT) and 298 K (RT), as shown in Figure 4. Based on the 113Cd NMR spectrum of solution T1 at 203 K, a mono(thiourea) cadmium(II) complex with δ = 93 ppm dominates in this solution, together with a minor amount of solvated Cd2+ ions and Cd(TU)22+ species (see below). Least squares curve-fitting to the k3-weighted EXAFS oscillation of T1 at LT with a model consisting of one Cd-S and five Cd-O scattering paths resulted in the mean distances 2.54 ± 0.02 Å and 2.30 ± 0.04 Å, respectively (Table 5). The number of bound TU / Cd(II) (= 1.06) from the peak integrals in the 113Cd NMR spectrum of solution T1 (Figure 1, middle) supports this model; see Appendix 2 in Supporting Information.

Figure 4.

Figure 4

Cd K-edge EXAFS (black lines) and curve-fitted model (red dashes) oscillations and corresponding Fourier-transforms for Cd(II)-thiourea complexes in methanol solutions (CCd(II) = 0.1 mol dm-3) with the mole ratios TU/ Cd(II) 1.0 (T1), 2.0 (T2), 4.0 (T4), 5.0 (T5), 8.0 (T6) and 10.0 (T7) measured at 200 K (LT) and 298 K (RT); see Table 5.

When increasing the thiourea concentration to 0.2 mol dm-3 in solution T2 (mole ratio TU / Cd(II) = 2.0), the 113Cd NMR spectrum indicated two major Cd(II) thiourea complexes with δ(113Cd) = 94 and 191 ppm beside a minor peak at 337 ppm (Figure 1). The FT peak position for the LT EXAFS spectrum for this solution shifted slightly to a longer distance and gained intensity (Figure 4). The LT EXAFS oscillation of this solution could be modeled with 2 Cd-S (2.55 ± 0.02 Å) and 4 Cd-O (2.33 ± 0.04 Å) scattering paths (Table 5). The peak integrals in the 113Cd NMR spectrum of solution T2 (Figure 1, middle) correspond to 2.17 bound TU / Cd(II) (see Appendix 2, Supporting Information). This ratio is higher than the stoichiometric TU / Cd(II) ratio (2.0), indicating an error of about 10% in the number estimated from the peak integrals. The EXAFS oscillation for solution T3 was not analyzed, as it contained several Cd(II) thiourea species beside the dominating one with δ(113Cd) = 191 ppm (Figure 1).

The highest FT amplitude in the LT EXAFS series T1 – T7 was obtained for solutions T4 and T5 with δ(113Cd) = 515 and 506 ppm, respectively. The LT EXAFS oscillations of these solutions were well modeled with four Cd-S distances at 2.53 – 2.54 Å. Attempts to include a Cd-O path resulted in too short Cd-O bond distances and/or unreasonable disorder parameters. With further increase in the thiourea concentration, from 0.5 mol dm-3 in T5 to 1.0 mol dm-3 in T7, the single 113Cd NMR signal shifted up-field from δ(113Cd) = 506 ppm to 423 ppm (Figure 1), with a considerable amplitude reduction of the LT EXAFS oscillations, as shown in Figure S-5 for solutions T4 and T7 with TU/Cd(II) mole ratios 4.0 and 10.0, respectively. This figure also shows that at 298 K the EXAFS spectra of these solutions (T4 and T7) overlap, which is consistent with their similar sharp 113Cd NMR peaks at 503 and 533 ppm, respectively (Figure 1, right), indicating that at room temperature the difference in speciation is not large enough to be distinguished by EXAFS spectroscopy.

The RT EXAFS oscillations for solutions T4 – T7 were well modeled with four Cd-S paths at 2.53 ± 0.02 Å (Table 5). A comparison of the EXAFS oscillations measured for solution T4 at two different temperatures (Figure S-6) shows similar frequencies, reflected in their similar bond distances (2.52 – 2.53 Å). However, the amplitude is higher at LT, resulting in slightly higher NCd-S (with fixed S02), and smaller σ2 values in the refinements. For solutions T1 and T2, for which no 113Cd NMR signal could be observed at RT, the EXAFS spectra had smaller amplitude at RT than at LT; see Figure S-6. For solution T2 the LT EXAFS oscillation had higher frequency, showing a significant shift to longer Cd-S bond distances from 2.51 Å at RT to 2.55 Å at LT, while the change in temperature did not influence the mean Cd-S and Cd-O bond distances for solution T1 (Table 5).

Cd K-edge EXAFS spectra for the Cd(II) thiourea aqueous solutions W1 – W7 were also measured and analyzed assuming mixtures of hydrated Cd(TU)x2+ (x = 1 - 4) species; see Figure S-1 and Table S-2.

X-ray absorption spectroscopy - Cd L3 -edge XANES

Cd L3-edge XANES spectroscopy has been shown to be sensitive to the type of coordinating atoms and the local coordination geometry around the cadmium(II) ion in its complexes. For example, Cd(II) complexes with CdO6 octahedral geometry show a distinct pre-edge feature at 3539.1 eV, originating from a core electron transition from Cd 2p3/2 to higher unoccupied molecular orbitals with s or d character.77,78,79 Therefore, Cd L3-edge XANES spectra were measured at room temperature of the Cd(II) thiourea solutions in methanol (T1 – T7) including Cd(CF3SO3)2 (model for CdO6), and for crystalline compounds with different CdSxOy coordination geometries (Figure 5). The XANES spectrum of solution T1 with a distinct pre-edge feature at 3539.1 eV resembles that of CdO6, while the second derivative of the spectral features for T2 is similar to those of CdS2O4. For solutions T4 – T7 the Cd L3-edge XANES features and corresponding 2nd derivatives are very similar, and comparable to the CdS4 model.

Figure 5.

Figure 5

Cd L3-edge XANES spectra at RT of the Cd(CF3SO3)2 -thiourea solutions in methanol T1 – T7, compared with Cd(CF3SO3)2 in methanol (CdO6) and crystalline standard compounds with CdSxOy coordination:79 [Cd(tmtu)2(NO3)2] (CdS2O4 model; tmtu = tetramethylthiourea),80 [Cd(DMTF)4(CF3SO3)2] (CdS4O2 model),48 [Cd(DMTF)6](ClO4)2 (CdS6 model),48 cadmium adamantane cage (Et3NH)4[S4Cd10(SPh)16] (CdS4 model),53 and (HIm)[Cd(tsac)3(H2O)] (CdS3O model; tsac = thiosaccharinato).49 The dashed lines are at 3539.1 and 3541.6 eV.

Discussion

Selenourea Cd(II) complex formation

The combined results from the 113Cd NMR and Cd K-edge EXAFS spectroscopic studies show a dominating mono-selenourea Cd(SeU)2+ complex with CdSeO5 coordination in the methanol solution S1 with mole ratio SeU/ Cd(II) = 1.0 (see Figures 1, 3 and Table 4). The O-donor ligands are methanol molecules and triflate ions, as in [Cd(DMTF)4(CF3SO3)2].48 For the mole ratios SeU / Cd(II) = 4.0 and 5.0 (solutions S4 and S5, respectively) a single cadmium(II)-selenourea complex [Cd(SeU)4]2+ with δ(113Cd) = 578 ppm dominates. The mean Cd-Se bond distance of 2.63 ± 0.02 Å (Table 4) is compatible with the average Cd-Se bond distances of 2.649 Å in [N(CH3)4]2[Cd(SePh)4],81 and 2.623 Å in [Cd(dmise)4][PF6]2, the only crystal structures with homoleptic CdSe4 coordination geometry.74 The synthesis of [Cd(SeU)4]SO4 was reported in 1972 without structural information.82 The 113Cd NMR chemical shift 541 ppm for the [Cd(SePh)4]2+ complex in methanol solution at 213 K,59 is slightly more shielded than that reported here of the [Cd(SeU)4]2+ complex at 203 K (Δδ = 578 – 541 = 37 ppm).

The slow ligand-exchange for the methanol solutions S1, S2 and S3 at 203 K allows the peaks observed at δ(113Cd) = 96-97, 193-194, 435 and 578 ppm (Figure 1), to be assigned to complexes with CdSeO5, CdSe2O4, CdSe3O and CdSe4 coordination, respectively. The relatively broad peaks prevented 113Cd-77Se coupling to be observed; such one-bond coupling normally is within 50 – 200 MHz.64 Previously, a 113Cd chemical shift of 250 ppm was obtained for a cadmium(II) selenocarboxylate complex with trigonal bipyramidal CdSe3O2 coordination geometry in CH2Cl2 at 193 K.64 A CSD survey did not show any crystalline compound with CdSe2O4 coordination, only one Cd(II) complex with CdSe2O3 coordination,83 and one monomeric CdSe3O complex with the Cd-Se bond distances within 2.590 – 2.603 Å and Cd-OH2 at 2.307 Å.84

By assuming that the integrated area of a distinct 113Cd NMR peak in Figure 1 is proportional to the concentration of a specific Cd(II) species in each cadmium(II) – selenourea (S1–S3) solution, the relative fractions (%Cd) and the formation constants of the Cd(II) species were evaluated (Table S-1b, Supporting Information). The formation constants (log βx, x = 1 - 4) of the Cd(SeU)x2+ species above were varied systematically until the distribution of complexes calculated in fraction diagrams approximately agreed with those obtained from the 113Cd NMR spectra; see Figure S-8 (top) in Appendix 1, Supporting Information. The evaluation showed that the log βx values are correlated with an estimated error limit of ±0.5 logarithmic units (Table 6).

Table 6.

Formation constants a of the Cd(II) selenourea / thiourea species CdLx2+ (L = SeU / TU, x = 1-4) formed in methanol solutions, derived from 113Cd NMR spectra at 203 K (see Figures 1, S-8 and S-9).

log βx (SeU) log βx (TU)
CdL2+ 4.4 4.3
CdL22+ 7.3 7.3
CdL32+ 10.7 9.7
CdL42+ 14.0 12.4
a

βx = [CdLx2+]/([Cd2+][L]x)

Thiourea Cd(II) complex formation in MeOH

Low temperature (~200 K)

In the 113Cd NMR spectra of the methanol solutions with TU / Cd(II) mole ratios 1.0, 2.0 and 3.0 (T1, T2 and T3), four peaks appeared at 203 K with δ = 93 – 94, 189 – 191, 333 – 337, and 526 ppm (Figure 1). A similar observation was reported for methanol solutions of Cd(ClO4)2 and 1,3-thiazolidine-2-thione (tztH) at 189 K with four peaks at -14, 73, 153, 453 ppm, which were tentatively assigned to solvated [Cd(tztH)w]2+ complexes with w = 0 - 3, respectively.46 For solution T1, the peak at 93 ppm has the highest intensity, and its Cd K-edge EXAFS spectrum is well modeled with one Cd-S and five Cd-O bond distances (2.54 ± 0.02 and 2.30 ± 0.04 Å, respectively; see Figure 4 and Table 5), showing that a mono(thiourea) Cd(II) complex with CdSO5 coordination (O from MeOH or CF3SO3-) dominates. For the methanol solution T2 with CCd(II) = 0.1 mol dm-3 and CTU = 0.2 mol dm-3, the 113Cd NMR signal at 191 ppm is the most intense (Figure 1). The average Cd-S and Cd-O bond distances 2.55 ± 0.02 Å and 2.33 ± 0.04 Å (Table 5) are comparable with the average Cd-S (2.585 Å) and Cd-O (2.366 Å) distances for the cis-[Cd(TU)2(H2O)4](SO4) complex,52 for which an isotropic solid state 113Cd NMR chemical shift of 148 ppm was observed (Figure S-4b). We conclude that a bis(thiourea)cadmium(II) complex, Cd(TU)22+, with a CdS2O4 coordination environment dominates in solution T2.

In solution T3 (TU/ Cd(II) mole ratio = 3.0), several species are in equilibrium giving rise to two sharp 113Cd NMR signals at 94 ppm (CdSO5) and 191 ppm (CdS2O4), and two broad peaks at 333 ppm and 526 ppm (Figure 1). The reported isotropic 113Cd NMR chemical shifts for complexes with CdS3O2 and CdS3O3 coordination (S = thiolate) vary within the range δiso = 390 – 410 ppm.85,86 Considering that the (HIm)[Cd(tsac)3(H2O)] and [Cd(TU)3(SO4)] complexes with CdS3O coordination, showed isotropic solid state 113Cd NMR chemical shifts at 378 and 346 ppm at room temperature, respectively (Figure S-4a, b), we can assign the peak at 333 ppm to tris(thiourea) Cd(II) complexes with CdS3O1-3 coordination in relatively fast ligand-exchange that broadens the peak. The broad peak at 526 ppm in the NMR spectrum of solution T3 can be assigned to a tetra(thiourea) Cd(II) complex mainly with CdS4 coordination (see Room temperature section).

Similar to the Cd(II)-selenourea system, the integrated peak areas in the 113Cd NMR spectra of the methanol solutions T1 – T3 at 203 K (Figure 1) were used to estimate the concentration of Cd(TU)y2+ (y = 1-4) species in each solution (Appendix 2, Supporting Information). The formation constants log βy were varied until the calculated fractions of Cd(TU)y2+ species in Figure S-9 (top) closely matched the fractions obtained from the peak areas (Table 6). The resulting βy values obtained for the solvated Cd(TU)y2+ (y = 1 – 4) species in methanol at 203 K (β1 = 2.0·104, β2 = 2.0·107, β3 = 5.0·109 and β4 = 2.5·1012) differ considerably from those previously reported from a polarographic study for similar complexes in aqueous solution at 298 K (β1 = 20, β2 = 140, β3 = 260 and β4 = 1200).16

By increasing the thiourea concentration from 0.4 mol dm-3 in T4 to 1.0 mol dm-3 in T7 (CCd(II) = 0.1 mol dm-3), the single 113Cd NMR peak became more shielded, shifting from 515 ppm in T4 to 423 ppm in T7. The latter value can be compared with δiso(113Cd) = 402 ppm recorded for crystalline [Cd(DMTF)6](ClO4)2 with octahedral CdS6 coordination (see Figure S-3). Therefore, the gradual shift of the NMR signal from 515 to 423 ppm is probably due to partial formation of Cd(II) complexes with a higher number of coordinated thiourea ligands, e.g. [Cd(TU)5]2+ (CdS5) and octahedral [Cd(TU)6]2+ (CdS6) species. Even though solution T7 has the highest thiourea concentration, the amplitude of its LT EXAFS oscillation is visibly smaller than that for T4 (Figure S-5 left).

An attempt to evaluate the speciation of the higher Cd(II)-thiourea complexes was made by fitting the LT EXAFS spectra for solutions T6 and T7 (TU / Cd(II) mole ratios 8.0 and 10.0, respectively) with linear combinations of EXAFS oscillations simulated for CdS4 and CdS6 coordination. The best fits shown in Figure 6 were obtained with the mean Cd-S distance 2.54 Å (σ2 = 0.005 Å2) for CdS4, and 2.71 Å (σ2 = 0.007 Å2) for CdS6, which are comparable with the mean Cd-S distance in crystalline [Cd(TU)4](NO3)2 with CdS4 coordination (2.53 ± 0.02 Å from EXAFS; Table 5 and Figure S-7), and 2.711 Å in a crystalline [Cd(TU)6]2+ complex with CdS6 coordination.15 Note that while the average of the crystallographic Cd-S distances in [Cd(TU)4](NO3)2 is 2.560 Å,13 the slightly shorter EXAFS value 2.53 ± 0.02 Å could result from a higher contribution from its short, more well-defined bond distances to the EXAFS oscillation. Ignoring a possible contribution from Cd(TU)52+ species, the linear combination fitting results in 77% contribution from CdS4 and 23% from CdS6 to the EXAFS oscillation for solution T6; for solution T7 the contributions are 68% CdS4 and 32% CdS6 (estimated error ± 10%). Figure 6 shows that the amplitude of the experimental EXAFS spectra is reduced by the opposing phases of the EXAFS oscillations for CdS4 and CdS6 coordination. Such a change in the Cd(II) speciation as in these solutions would have been difficult to interpret solely based on EXAFS spectroscopy, without the aid from the 113Cd NMR spectra.

Figure 6.

Figure 6

Cd K-edge EXAFS spectra at LT for the Cd(II) thiourea methanol solutions T6 and T7 fitted with linear combinations of simulated EXAFS oscillations for CdS4 and CdS6 coordination, indicating more than four thiourea ligands in ~ 20 – 30% of the cadmium(II) complexes.

Room temperature

For the cadmium(II) thiourea solutions T1 – T3, for which no 113Cd NMR signal could be observed at 295 K, the Cd L3-edge XANES spectral features were useful for indicating the coordination of the major cadmium(II) species. The Cd L3-edge XANES spectrum of T1 resembles that of Cd(CF3SO3)2 in methanol (CdO6 model) in Figure 5. At LT the 113Cd NMR spectrum showed that some free solvated Cd2+ ions were present (Figure 1). The RT EXAFS spectrum of solution T1 could be fitted with a CdSO5 model with the average Cd-O and Cd-S distances 2.30 ± 0.02 Å and 2.54 ± 0.02 Å, respectively, which are comparable to those obtained for this solution at LT (see Table 5 and Figure S-6). The resemblance between the Cd L3-edge XANES spectra of solution T2 and the CdS2O4 model in Figure 5, and also the corresponding second derivatives, implies that solution T2 mainly contains the bis(thiourea)cadmium(II) complex as the dominating species. Fitting the RT Cd K-edge EXAFS spectrum of solution T2 with a CdS2O4 model resulted in a somewhat shorter average Cd-S distance 2.51 ± 0.02 Å.

The 113Cd NMR spectra of solutions T4 – T7 with TU / Cd(II) mole ratios 4.0 – 10.0 showed at 295 K a single sharp peak in the 503 – 541 ppm region. The RT EXAFS spectra of these solutions almost overlap (Figure S-5, right), and were well fitted with a CdS4 model with an average Cd-S distance of 2.52 – 2.53 Å. The second derivatives of their Cd L3-edge absorption spectra showed two minima, rather similar to those observed for the CdS4 model compound (Figure 5). Thus, at high thiourea concentration (TU / Cd(II) > 4.0) the [Cd(TU)4]2+ complex dominates at room temperature. Reducing the temperature of these solutions (T5 – T7) to ~200 K promotes the formation of CdS5-6 complexes, resulting in longer average Cd-S distances (up to 2.55 Å for T7) and more shielded 113Cd chemical shifts (423 ppm for T7).

For the crystalline [Cd(TU)4](NO3)2 complex with an average Cd-S distance of 2.53 ± 0.02 Å (from EXAFS; see Table 5 and Figure S-7), a solid state 113Cd NMR isotropic chemical shift of δiso = 577 ppm was obtained (Figure S-3), while the 113Cd NMR chemical shift for [Cd(TU)4]2+ ions in methanol solution is more shielded (541 ppm at 295 K). A similar up-field shift has been reported for [Cd(Se-2,4,6-iPr3-C6H2)2(bpy)] complex (δiso = 460, 472) when dissolved in chloroform (411 ppm),61 and was explained as a “solvent effect” (see Table 2).

Based on the above discussion, the broad peak at 526 ppm in the LT 113Cd NMR spectrum of solution T3 can be assigned to [Cd(TU)4]2+ species with rather slow ligand-exchange on the NMR scale. The broadness of this peak could be due to a minor amount of a Cd(II) tetra(thiourea) complex with CdS4O coordination. Higher O-donor ligand coordination is not likely, since the chemical shift becomes more shielded, e.g. for [Cd(DMTF)4(CF3SO3)2] with CdS4O2 coordination, δiso (113Cd) = 267 ppm (Table 1). The isotropic chemical shifts for CdS4 and CdS4O coordination (S = thiolate) in the [Cd10(SCH2CH2OH)16](ClO4)4 compound were reported at 674 and 503 ppm, respectively.87,* The 113Cd NMR chemical shifts measured at room temperature for the [Cd(TU)4]2+ complex (CdS4 coordination) in the solid state (δiso = 577 ppm) and in methanol solution (541 ppm) are more shielded than that for mononuclear Cd(II)-tetrathiolate complexes (~600 - 750 ppm).43

Thiourea Cd(II) complex formation in H2O

The cadmium(II) complex formation with thiourea in aqueous solution was also investigated at room temperature, keeping the same cadmium(II) concentration as for the methanol solutions (~0.1 mol dm-3 Cd(CF3SO3)2), with the TU concentration varying from 0.1 to 2.0 mol dm-3 (W1 – W9, Table 3). The single sharp peak with a gradual downfield shift from 60 ppm (W1) to 446 ppm (W9) in the 113Cd NMR spectra shown in Figure 2 corresponds to cadmium(II) complexes with an increasing number of coordinated thiourea ligands in fast ligand exchange, as the TU concentration increases. A similar trend is also observed for the isotropic 113Cd NMR chemical shifts with δiso = 148, 346 and 577 ppm of the cis-[Cd(TU)2(H2O)4](SO4), [Cd(TU)3(SO4)] and [Cd(TU)4](NO3)2 solid compounds, respectively (Table 1).

The Cd K-edge EXAFS spectra for the aqueous solutions W1 – W7 were analyzed (Table S-2), keeping the average Cd-S and Cd-O coordination numbers fixed at values derived from the calculated distribution of complexes assuming [Cd(TU)y(H2O)6-y]2+ (y = 0 – 3) and [Cd(TU)4]2+ species (Figure S-1); the results showed a mean Cd-S distance of about 2.54 - 2.57 Å for solutions W1 to W5. The mean Cd-S distance became slightly shorter, about 2.53 Å, for solutions W6 and W7 (TU / Cd mole ratios 8.0 and 10.0, respectively), while the mean of the Cd-O distances is around 2.28 ± 0.04 Å for all solutions (Table S-2). This trend corresponds to that expected for hydrated [Cd(TU)(H2O)5]2+ and [Cd(TU)2(H2O)4]2+ complexes in a mixture, with a gradually increasing amount of [Cd(TU)4]2+ complexes without coordinated water (Figure S-1). The crystal structure of a hydrated cadmium thiourea sulfate showed both cis-[Cd(TU)2(H2O)4](SO4) and fac-[Cd(TU)3(H2O)3](SO4) complexes co-crystallized in the unit cell, with the mean Cd-S (Cd-O) bond distances 2.59 (2.37) Å and 2.62 (2.41) Å, respectively.52 A mean Cd-S distance of 2.53 ± 0.02 Å is expected for a [Cd(TU)4]2+ complex from EXAFS, as obtained for the solid [Cd(TU)4](NO3)2 compound (Table 5 and Figure S-7).

Therefore, we interpret the combined results of the aqueous solutions W1 – W5 (CCd(II) = 0.1 mol dm-3 and TU/ Cd(II) = 1.0 – 5.0) as corresponding to dominating hydrated [Cd(TU)(H2O)5]2+ and [Cd(TU)2(H2O)4]2+ complexes that are in fast ligand exchange on the NMR time scale. By further increasing the thiourea concentration in solutions W6 to W9 (mole ratios TU / Cd(II) = 8.0 to 20.0, respectively) the tetrahedral [Cd(TU)4]2+ complex becomes the dominant species, shifting the 113Cd NMR signal downfield. When compared to the 113Cd NMR spectra of the methanol solutions T4 – T7 measured at room temperature (Figure 1, right), it is evident that the [Cd(TU)4]2+ complex dominates already at the mole ratio TU / Cd(II) = 4.0 in methanol, which is a much weaker ligand than water. We are unable to ascertain the degree of hydration m in the [Cd(TU)3(H2O)m]2+ complex, which is a minor species in solution according to the stability constants (Figure S-1), but propose that the [Cd(TU)3(H2O)3]2+ complex is formed, as in the crystal structure.52

Comparison between Cd(II) complex formation with selenourea and thiourea in MeOH at ~200 K

The 113Cd NMR spectra of 0.1 mol dm-3 Cd(CF3SO3)2 solutions (Figure 1) in methanol containing 0.1 – 0.3 mol dm-3 selenourea (S1 – S3) or thiourea (T1 – T3) at 203 K show similar peaks in the 93 – 97 ppm and 189 – 194 ppm range, which were assigned to complexes with Cd(Se/S)O5 and Cd(Se/S)2O4 coordination geometries, respectively. In this case the chemical shifts are very similar when one or two S / Se-donor ligands replace the O-donor ligands (methanol and CF3SO3- in the current case), in contrast to the generally observed trend with decreasing shielding of donor atoms in the order: O ≫ Se > S.43 Also the formation constants for the CdL2+ and CdL22+ species are virtually the same for the SeU and TU systems, while Cd(SeU)32+ and Cd(SeU)42+ are more stable than the corresponding Cd(TU)32+ and Cd(TU)42+ complexes. The tris(thiourea)cadmium(II) complexes, Cd(TU)32+, with CdS3O1-3 coordination give rise to broad peaks at 333 - 337 ppm in the 113Cd NMR spectra of the T2 – T3 solutions, while the tris(selenourea)cadmium(II) complexes with tetrahedral CdSe3O coordination correspond to the relatively sharp peak at 435 ppm, as for solutions S1 – S3. In the methanol solutions S4 and S5, containing 0.4 – 0.5 mol dm-3 selenourea, respectively, a [Cd(SeU)4]2+ complex with a CdSe4 core is predominantly present. Its chemical shift δ(113Cd) = 578 ppm is comparable to δiso = 577 ppm observed for CdS4 coordination in the solid state 113Cd NMR spectrum of [Cd(TU)4](NO3)2 (Figure S-3), and is more deshielded than that of [Cd(TU)4]2+ (CdS4, 526 ppm) in methanol solution at 203 K. Likewise, Isab and coworkers reported a more deshielded solid state 113Cd NMR isotropic chemical shift for Cd(SeU)2Cl2 (458 ppm) than that for Cd(TU)2Cl2 (430 ppm).36 The rather broad peak at 515 ppm for solution T4, containing 0.4 mol dm-3 thiourea, indicates that the [Cd(TU)4]2+ complex dominates; however, by increasing the ligand concentration higher complexes with CdS5-6 coordination are formed.

Conclusion

In the current study, we have made a detailed evaluation of the speciation of cadmium(II) complexes with selenourea and thiourea by varying the ligand concentration, solvent and temperature using a combination of spectroscopic methods, 113Cd NMR, Cd K-edge EXAFS and Cd L-edge XANES. In methanol solutions of 0.1 mol dm-3 Cd(CF3SO3)2 with mole ratios L / Cd(II) ≤ 3.0 (L = SeU, TU), 113Cd NMR spectroscopy shows mixtures of CdLn2+ (n = 1 – 4) species in slow ligand exchange equilibria at 203 K, which allowed their stability constants to be estimated. In ligand excess tetrahedral [Cd(SeU)4]2+ and [Cd(TU)4]2+ complexes dominate at 203 K and 295 K, respectively, with the average bond distances Cd-Se 2.63 ± 0.02 Å and Cd-S 2.53 ± 0.02 Å, as determined by Cd K-edge EXAFS spectroscopy. When lowering the temperature from 295 K to 203 K for 0.1 mol dm-3 Cd(CF3SO3)2 methanol solutions with high mole ratios, TU / Cd(II) > 5.0, complexes with even higher thiourea coordination, [Cd(TU)5-6]2+, form to some extent.

In aqueous solutions of 0.1 mol dm-3 Cd(CF3SO3)2 with increasing thiourea concentration the 113Cd NMR signal at 295 K corresponds to mixtures of [Cd(TU)y(H2O)6-y]2+ (y = 0 – 3) species in fast ligand exchange equilibria with [Cd(TU)4]2+ complexes. Higher excess of the thiourea ligand is needed than in comparable methanol solutions to form the [Cd(TU)4]2+ complex, which becomes the major species for free concentrations of thiourea exceeding ~0.4 mol dm-3.

Based on the 113Cd NMR chemical shifts observed in this study, Se (selone) and S (thione) donor atoms provide similar shielding effects in Cd(II) selenourea and thiourea complexes with similar coordination geometries. Almost identical δ(113Cd) chemical shifts were observed at 203 K for the octahedrally coordinated Cd(Se/S)O5 (δ ~ 95 ppm) and Cd(Se/S)2O4 species (δ ~ 190 ppm), with MeOH and possibly CF3SO3- as O-donor ligands. For the [Cd(SeU)4]2+ complex (CdSe4 coordination) the chemical shift recorded at 578 ppm (MeOH, 203 K) is somewhat more deshielded than that of [Cd(TU)4]2+ (CdS4 coordination, 526 ppm in MeOH at 203 K), although close to the isotropic chemical shift δiso (113Cd) = 577 ppm for crystalline [Cd(TU)4](NO3)2 measured at room temperature (Table 1).

When reporting 113Cd NMR shifts the coordination geometry is well defined for crystalline Cd(II) complexes; however, in solution the structure will not necessarily stay the same. Our method using X-ray absorption spectroscopy as a supporting tool to further characterize the cadmium(II) species in solution significantly increases the insight in the systems studied. We have shown that 113Cd NMR spectroscopy can be used for quite detailed speciation at LT in methanol solution, where for example the EXAFS technique was unable on its own to ascertain the partial formation of [Cd(TU)5-6]2+ complexes, as the overall increase in the Cd-S bond distances was ~ 0.02 Å, within the error limit of EXAFS spectroscopy. Conversely XAS spectroscopy was needed to structurally characterize the dominating species in the methanol solutions, especially to confirm that the Cd(II)-thiourea species with δ(113Cd) = 526 ppm (541 ppm at 295 K) indeed is the [Cd(TU)4]2+ complex (CdS4 coordination), which surprisingly has a more shielded chemical shift than [Cd(SeU)4]2+ with δ(113Cd) = 578 ppm and CdSe4 coordination.

We also show that thiourea, as a model for thione-containing ligands with neutral S-donor atoms, is more shielding than the thiolate groups with negatively charged S-donors, when comparing [Cd(TU)4]2+ with δ(113Cd) = 541 ppm (in MeOH at 295 K) with the reported chemical shifts for Cd(II)-tetrathiolates (~ 600 - 750 ppm). Therefore, caution should be exercised when interpreting sulfur coordination in biological systems based on 113Cd NMR chemical shifts.

The individual chemical shifts obtained here are useful additions to the 113Cd NMR chemical shifts previously reported for Cd(II)-thione complexes (Table 1), as well as cadmium(II) complexes with Se-donor ligands (Table 2). The 113Cd NMR chemical shifts reported for cadmium(II) complexes with Se-donor ligands in general are altogether quite few,88 as also the crystal structures when compared with S-donor ligands, probably due to the air-sensitivity of most organo-selenium compounds.

Supplementary Material

1_si_001

Acknowledgments

We are grateful to Qiao Wu, Dorothy Fox and Jian Jun Li at the instrument facility at the Department of Chemistry, University of Calgary, for their skilful assistance in measuring the NMR spectra. Special thanks to Eun Young Kang for preparing the aqueous Cd(II) thiourea solutions (W1 – W7). Beam time was allocated for X-ray absorption measurements at SSRL (proposal No. 2848), which is operated by the Department of Energy, Office of Basic Energy Sciences, USA. The SSRL Biotechnology Program is supported by the National Institutes of Health, National Center for Research Resources, Biomedical Technology Program, and by the Department of Energy, Office of Biological and Environmental Research. We gratefully acknowledge the Natural Sciences and Engineering Council (NSERC) of Canada, Canadian Foundation for Innovation (CFI), Alberta Science and Research Investments Program (ASRIP) and the University of Calgary for providing financial support.

Footnotes

*

The sign of the chemical shifts is changed; also the calibration is shifted by changing δiso for the solid reference compound Cd(NO3)2.4H2O from 0.0 ppm to -100 ppm.

Supporting Information Available. Total number of 113Cd NMR scans collected for each sample and integrated peak areas for solutions T1 – T3 and S1 – S3, solid state 113Cd NMR spectra for crystalline Cd(TU)4(NO3)2, Cd(DMTF)6(ClO4)2, Cd(DMTF)4(CF3SO3)2, (HIm)[Cd(tsac)3(H2O)] and [Cd(TU)3(SO4)], comparison between Cd K-edge EXAFS spectra of solutions T4 and T7 at LT / RT, comparison between the EXAFS spectra measured at 200 K and 298 K for solutions T1, T2 and T4, EXAFS curve-fitting results for the aqueous Cd(II)-thiourea solutions W1 – W7, a diagram showing the fractions of Cd(TU)x2+ (x = 0 – 4) species formed in aqueous solution vs. total thiourea concentration, calculations regarding the average number of TU (/ SeU) per Cd(II) ion in solutions S1 – S3 and T1 – T3, and fraction diagrams displaying the calculated distribution of Cd(TU)x and Cd(SeU)x (x = 0 – 4) species in methanol vs. total TU or SeU concentration, respectively. This material is available free of charge via the Internet at http://pubs.acs.org.

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