metal-organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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Di­chlorido­[2-(pyridin-2-yl-κN)-1,5-naphthyridine-κN1]zinc(II)

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aGraduate School of Science and Engineering, University of Toyama, 3190 Gofuku, Toyama 930-8555, Japan
*Correspondence e-mail: [email protected]

Edited by M. Bolte, Goethe-Universität Frankfurt, Germany (Received 25 August 2025; accepted 27 August 2025; online 5 September 2025)

The title zinc(II) complex, [ZnCl2(C13H9N3)], crystallizes in the triclinic space group P1. The coordination environment around the zinc(II) ion in the title complex can be described as a distorted tetra­hedron formed by the two N atoms of the NAD+/NADH model ligand pn [pn = 2-(pyridin-2-yl)[1,5]naphthyridine] and two Cl ions. There are ππ stacking inter­actions in the crystal packing of the title compound.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

Photo-driven carbon dioxide (CO2) reduction has been one of the most attractive approaches to address global energy and environmental problems because of its capacity to transform CO2 into value-added chemical compounds, such as formic acid and carbon monoxide, under mild conditions by utilizing solar energy (Wang et al., 2022View full citation). Transition-metal mol­ecular catalysts are an important tool and play a central role in the roadmap to achieve efficient and novel CO2 photoreduction into valuable chemicals (Kumagai et al., 2022View full citation). Our motivation for investigating transition-metal complexes with a coenzyme NAD+/NADH model ligand is based on their potential as candidates for photocatalytic CO2 reduction. The synthesis and use of the NAD+/NADH model ligand pbn [pbn = 2-(pyridin-2-yl)benzo[b][1,5]naphthyridine] was first reported by Koizumi & Tanaka (2005View full citation), and we have previously developed a novel photocatalytic CO2 reduction process to produce formic acid using a Ru-based pbn complex (Ohtsu & Tanaka, 2012View full citation; Ohtsu et al., 2015View full citation, 2019View full citation).

In order to further develop transition-metal NAD+/NADH model complexes, substituent tuning of NAD+/NADH model ligands offers a potentially powerful means not only to control catalytic activity of the complexes but also to confer new reactivity on the complexes. However, the synthetic pathway to introduce substituents into the benzonaphthyridine skeleton of the pbn ligand is considerably difficult.

As part of our ongoing investigation of transition-metal complexes bearing various substituted NAD+/NADH model ligands, we have focused on the non-substituted NAD+/NADH model ligand pn [pn = 2-(pyridin-2-yl)[1,5]naphthyridine] synthesized by Singh & Thummel (2009View full citation), which can possess the potential to facilitate the introduction of substituents through a straightforward synthetic process. A new zinc(II) complex with a pn ligand has been structurally characterized and is reported in this paper.

The mol­ecular structure of the title complex, [ZnCl2(pn)], is shown in Fig. 1[link] and selected geometrical data are listed in Table 1[link]. The zinc(II) ion in [ZnCl2(pn)] has a tetra­coordinate structure formed by the two N atoms of pn ligand [Zn1—N2 = 2.0909 (14) Å, Zn1—N3 = 2.0560 (14) Å] and two Cl ions [Zn1—Cl1 = 2.2137 (6) Å, Zn1—Cl2 = 2.2161 (6) Å]. The qu­anti­tative difference in four-coordinate geometry is indicated by an index of τ4. The value can range from τ4 = 1 for a perfect tetra­hedral geometry to τ4 = 0 for a perfect square planar geometry (Yang et al., 2007View full citation). The τ4 value for the zinc(II) ion of the title complex is obtained as τ4 = 0.88 by using the equation τ4 = [360–(α+β)]/141 (Yang et al., 2007View full citation), where α = N3—Zn1—Cl2 [120.94 (4)°], β = Cl1—Zn1—Cl2 [114.81 (2)°]. Thus, the coordination environment of the zinc(II) ion in [ZnCl2(pn)] is a slightly distorted tetra­hedron. The pyridine ring and the naphthyridine ring system in the pn ligand are twisted to give a dihedral angle of 10.57 (5)° between the two least-squares planes.

Table 1
Selected geometric parameters (Å, °)

Zn1—N3 2.0560 (14) Zn1—Cl1 2.2137 (6)
Zn1—N2 2.0909 (14) Zn1—Cl2 2.2161 (6)
       
N3—Zn1—N2 79.59 (6) N3—Zn1—Cl2 120.94 (4)
N3—Zn1—Cl1 113.63 (4) N2—Zn1—Cl2 108.77 (4)
N2—Zn1—Cl1 113.74 (4) Cl1—Zn1—Cl2 114.81 (2)
[Figure 1]
Figure 1
The mol­ecular structure of the title compound with displacement ellipsoids for non-hydrogen atoms at the 50% probability level.

The crystal packing of the title complex is shown in Fig. 2[link]. There are noteworthy ππ stacking inter­actions between neighboring naphthyridine ring systems of the pn ligand, with a centroid–centroid distance of 3.625 (1) Å. No other significant or inter­esting inter­molecular inter­actions are observed.

[Figure 2]
Figure 2
Part of the crystal structure showing a ππ inter­action (red dotted line). Zn atoms are represented in yellow, Cl in green, N in blue, and C in gray. Hydrogen atoms are omitted for clarity.

Synthesis and crystallization

The NAD+/NADH model ligand, 2-(pyridin-2-yl)[1,5]naphthyridine abbreviated as pn, was prepared according to the literature procedure (Singh & Thummel, 2009View full citation).

To a di­chloro­methane solution (4.0 ml) of pn (36.44 mg, 17.6 mmol) was added dropwise ZnCl2 (23.95 mg, 17.6 mmol) in aceto­nitrile (4.0 ml), and the resulting solution was left to stand for a few days at room temperature. Light-yellow crystals of the title compound [ZnCl2(pn)] were obtained (yield; 44.48 mg, 73.7%). Elemental analysis, found: C 45.32, H 2.69, N 12.18%; calculated for C13H9Cl2N3Zn: C 45.45, H 2.64, N 12.23%.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula [ZnCl2(C13H9N3)]
Mr 343.52
Crystal system, space group Triclinic, PMathematical equation
Temperature (K) 173
a, b, c (Å) 8.0634 (15), 8.6146 (17), 10.2087 (19)
α, β, γ (°) 86.492 (6), 78.622 (6), 70.336 (5)
V3) 654.6 (2)
Z 2
Radiation type Mo Kα
μ (mm−1) 2.27
Crystal size (mm) 0.23 × 0.11 × 0.07
 
Data collection
Diffractometer Rigaku R-AXIS RAPID
Absorption correction Multi-scan (ABSCOR; Rigaku, 1995View full citation)
Tmin, Tmax 0.630, 0.853
No. of measured, independent and observed [F2 > 2.0σ(F2)] reflections 6486, 2992, 2693
Rint 0.034
(sin θ/λ)max−1) 0.649
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.026, 0.069, 1.03
No. of reflections 2992
No. of parameters 172
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.43, −0.28
Computer programs: RAPID-AUTO (Rigaku, 2001View full citation), SHELXT2018/2 (Sheldrick, 2015aView full citation), SHELXL2019/3 (Sheldrick, 2015bView full citation), CrystalStructure (Rigaku, 2019View full citation), CrystalMaker (Palmer, 2014View full citation) and publCIF (Westrip, 2010View full citation).

Structural data


Computing details top

Dichlorido[2-(pyridin-2-yl-κN)-1,5-naphthyridine-κN1]zinc(II) top
Crystal data top
[ZnCl2(C13H9N3)]Z = 2
Mr = 343.52F(000) = 344.00
Triclinic, P1Dx = 1.743 Mg m3
a = 8.0634 (15) ÅMo Kα radiation, λ = 0.71075 Å
b = 8.6146 (17) ÅCell parameters from 4464 reflections
c = 10.2087 (19) Åθ = 2.0–27.5°
α = 86.492 (6)°µ = 2.27 mm1
β = 78.622 (6)°T = 173 K
γ = 70.336 (5)°Block, colorless
V = 654.6 (2) Å30.23 × 0.11 × 0.07 mm
Data collection top
Rigaku R-AXIS RAPID
diffractometer
2693 reflections with F2 > 2.0σ(F2)
Detector resolution: 10.000 pixels mm-1Rint = 0.034
ω scansθmax = 27.5°, θmin = 2.5°
Absorption correction: multi-scan
(ABSCOR; Rigaku, 1995)
h = 1010
Tmin = 0.630, Tmax = 0.853k = 1111
6486 measured reflectionsl = 1312
2992 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.026Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.069H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0387P)2 + 0.1345P]
where P = (Fo2 + 2Fc2)/3
2992 reflections(Δ/σ)max = 0.001
172 parametersΔρmax = 0.43 e Å3
0 restraintsΔρmin = 0.28 e Å3
Primary atom site location: structure-invariant direct methods
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. Refinement was performed using all reflections. The weighted R-factor (wR) and goodness of fit (S) are based on F2. R-factor (gt) are based on F. The threshold expression of F2 > 2.0 sigma(F2) is used only for calculating R-factor (gt).

H atoms were located in a difference map and refined as riding on their parent atoms with C–H = 0.95 Å and with Uiso(H) = 1.2 Ueq(C).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Zn10.52702 (3)0.80210 (2)0.18747 (2)0.02563 (8)
Cl10.70577 (6)0.89381 (6)0.27656 (5)0.03363 (12)
Cl20.29182 (6)0.99685 (6)0.13125 (5)0.03711 (12)
N10.1233 (2)0.5604 (2)0.59856 (15)0.0327 (3)
N20.43844 (18)0.62744 (18)0.30470 (13)0.0220 (3)
N30.66057 (19)0.59482 (18)0.07077 (14)0.0235 (3)
C10.0609 (2)0.7111 (3)0.64747 (18)0.0326 (4)
H10.0293640.7326080.7258850.039*
C20.1173 (2)0.8429 (2)0.59282 (18)0.0305 (4)
H20.0685030.9480330.6350550.037*
C30.2437 (2)0.8172 (2)0.47777 (18)0.0284 (4)
H30.2841410.9038860.4380310.034*
C40.3122 (2)0.6578 (2)0.41992 (16)0.0227 (3)
C50.2495 (2)0.5333 (2)0.48381 (16)0.0250 (3)
C60.3234 (2)0.3738 (2)0.42718 (18)0.0287 (4)
H60.2849850.2866710.4683300.034*
C70.4511 (2)0.3448 (2)0.31252 (17)0.0259 (3)
H70.5018270.2378540.2734900.031*
C80.5059 (2)0.4762 (2)0.25336 (15)0.0215 (3)
C90.6415 (2)0.4540 (2)0.12667 (15)0.0218 (3)
C100.7425 (2)0.3016 (2)0.06984 (18)0.0280 (4)
H100.7283080.2037570.1110030.034*
C110.8650 (2)0.2936 (2)0.04844 (18)0.0303 (4)
H110.9371520.1898430.0880500.036*
C120.8812 (2)0.4371 (2)0.10788 (17)0.0291 (4)
H120.9616600.4344320.1900110.035*
C130.7767 (2)0.5854 (2)0.04455 (17)0.0280 (4)
H130.7880060.6846660.0846770.034*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn10.02615 (12)0.01684 (12)0.03053 (12)0.00643 (9)0.00227 (9)0.00346 (8)
Cl10.0383 (2)0.0267 (2)0.0385 (2)0.01520 (19)0.0046 (2)0.00282 (18)
Cl20.0341 (2)0.0217 (2)0.0473 (3)0.00115 (18)0.0029 (2)0.00052 (19)
N10.0306 (8)0.0319 (9)0.0285 (7)0.0073 (7)0.0053 (7)0.0006 (6)
N20.0207 (6)0.0200 (7)0.0236 (6)0.0062 (5)0.0003 (6)0.0030 (5)
N30.0251 (7)0.0181 (7)0.0247 (6)0.0057 (6)0.0007 (6)0.0010 (5)
C10.0269 (9)0.0360 (11)0.0263 (8)0.0041 (8)0.0039 (7)0.0017 (7)
C20.0252 (8)0.0295 (10)0.0309 (9)0.0023 (7)0.0014 (7)0.0085 (7)
C30.0275 (8)0.0243 (9)0.0308 (9)0.0075 (7)0.0003 (8)0.0046 (7)
C40.0188 (7)0.0239 (9)0.0234 (8)0.0049 (6)0.0030 (7)0.0015 (6)
C50.0230 (8)0.0258 (9)0.0232 (7)0.0058 (7)0.0023 (7)0.0019 (6)
C60.0322 (9)0.0226 (9)0.0301 (8)0.0106 (7)0.0015 (8)0.0038 (7)
C70.0292 (8)0.0187 (8)0.0268 (8)0.0052 (7)0.0032 (7)0.0004 (6)
C80.0211 (7)0.0198 (8)0.0221 (7)0.0053 (6)0.0035 (7)0.0001 (6)
C90.0220 (7)0.0205 (8)0.0219 (7)0.0060 (6)0.0031 (7)0.0011 (6)
C100.0322 (9)0.0195 (9)0.0295 (8)0.0071 (7)0.0010 (8)0.0019 (7)
C110.0299 (9)0.0236 (9)0.0318 (9)0.0049 (7)0.0023 (8)0.0073 (7)
C120.0272 (8)0.0311 (10)0.0250 (8)0.0081 (7)0.0024 (7)0.0034 (7)
C130.0298 (9)0.0247 (9)0.0271 (8)0.0094 (7)0.0005 (7)0.0013 (7)
Geometric parameters (Å, º) top
Zn1—N32.0560 (14)C4—C51.408 (2)
Zn1—N22.0909 (14)C5—C61.410 (3)
Zn1—Cl12.2137 (6)C6—C71.371 (2)
Zn1—Cl22.2161 (6)C6—H60.9500
N1—C11.314 (3)C7—C81.410 (2)
N1—C51.366 (2)C7—H70.9500
N2—C81.328 (2)C8—C91.496 (2)
N2—C41.369 (2)C9—C101.382 (2)
N3—C131.340 (2)C10—C111.390 (2)
N3—C91.352 (2)C10—H100.9500
C1—C21.406 (3)C11—C121.378 (3)
C1—H10.9500C11—H110.9500
C2—C31.369 (3)C12—C131.386 (3)
C2—H20.9500C12—H120.9500
C3—C41.414 (2)C13—H130.9500
C3—H30.9500
N3—Zn1—N279.59 (6)N1—C5—C6119.26 (16)
N3—Zn1—Cl1113.63 (4)C4—C5—C6117.99 (15)
N2—Zn1—Cl1113.74 (4)C7—C6—C5119.77 (16)
N3—Zn1—Cl2120.94 (4)C7—C6—H6120.1
N2—Zn1—Cl2108.77 (4)C5—C6—H6120.1
Cl1—Zn1—Cl2114.81 (2)C6—C7—C8119.04 (16)
C1—N1—C5116.46 (16)C6—C7—H7120.5
C8—N2—C4119.22 (14)C8—C7—H7120.5
C8—N2—Zn1114.20 (11)N2—C8—C7122.39 (15)
C4—N2—Zn1126.40 (11)N2—C8—C9115.80 (14)
C13—N3—C9118.69 (15)C7—C8—C9121.80 (15)
C13—N3—Zn1126.24 (12)N3—C9—C10121.59 (15)
C9—N3—Zn1114.60 (11)N3—C9—C8115.16 (14)
N1—C1—C2125.12 (17)C10—C9—C8123.25 (15)
N1—C1—H1117.4C9—C10—C11119.02 (16)
C2—C1—H1117.4C9—C10—H10120.5
C3—C2—C1118.96 (17)C11—C10—H10120.5
C3—C2—H2120.5C12—C11—C10119.61 (17)
C1—C2—H2120.5C12—C11—H11120.2
C2—C3—C4117.95 (17)C10—C11—H11120.2
C2—C3—H3121.0C11—C12—C13118.17 (16)
C4—C3—H3121.0C11—C12—H12120.9
N2—C4—C5121.59 (15)C13—C12—H12120.9
N2—C4—C3119.67 (16)N3—C13—C12122.88 (17)
C5—C4—C3118.74 (15)N3—C13—H13118.6
N1—C5—C4122.75 (16)C12—C13—H13118.6
C5—N1—C1—C21.7 (3)C4—N2—C8—C9179.39 (14)
N1—C1—C2—C31.8 (3)Zn1—N2—C8—C93.94 (17)
C1—C2—C3—C40.4 (3)C6—C7—C8—N20.0 (3)
C8—N2—C4—C51.3 (2)C6—C7—C8—C9178.65 (15)
Zn1—N2—C4—C5173.50 (12)C13—N3—C9—C102.0 (2)
C8—N2—C4—C3177.99 (15)Zn1—N3—C9—C10170.68 (13)
Zn1—N2—C4—C37.2 (2)C13—N3—C9—C8178.52 (15)
C2—C3—C4—N2179.83 (15)Zn1—N3—C9—C88.83 (18)
C2—C3—C4—C50.8 (2)N2—C8—C9—N38.6 (2)
C1—N1—C5—C40.3 (3)C7—C8—C9—N3170.21 (15)
C1—N1—C5—C6179.19 (17)N2—C8—C9—C10170.93 (15)
N2—C4—C5—N1179.78 (16)C7—C8—C9—C1010.3 (2)
C3—C4—C5—N10.9 (2)N3—C9—C10—C110.7 (3)
N2—C4—C5—C61.4 (2)C8—C9—C10—C11179.82 (16)
C3—C4—C5—C6177.98 (16)C9—C10—C11—C121.2 (3)
N1—C5—C6—C7179.57 (16)C10—C11—C12—C131.8 (3)
C4—C5—C6—C70.7 (3)C9—N3—C13—C121.4 (3)
C5—C6—C7—C80.0 (3)Zn1—N3—C13—C12170.35 (13)
C4—N2—C8—C70.6 (2)C11—C12—C13—N30.5 (3)
Zn1—N2—C8—C7174.83 (13)
Selected geometric parameters (Å, °) top
Zn1–N22.0909 (14)Zn1–Cl12.2137 (6)
Zn1–N32.0560 (14)Zn1–Cl22.2161 (6)
N2–Zn1–Cl1113.74 (4)N3–Zn1–Cl1113.63 (4)
N2–Zn1–Cl2108.77 (4)N3–Zn1–Cl2120.94 (4)
N2–Zn1–N379.59 (6)
 

Funding information

This work was supported by Grants-in-Aid for Scientific Research (C) (22K05126, to HO) from the Ministry of Education, Culture, Sports, Science, and Technology (MEXT) and Japan Society for the Promotion of Science (JSPS).

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