New Dinuclear Macrocyclic Copper(II) Complexes as Potentially Fluorescent and Magnetic Materials

Two dinuclear copper(II) complexes with macrocyclic Schiff bases K1 and K2 were prepared by the template reaction of (R)-(+)-1,1′-binaphthalene-2,2′-diamine and 2-hydroxy-5-methyl-1,3-benzenedicarboxaldehyde K1, or 4-tert-butyl-2,6-diformylphenol K2 with copper(II) chloride dihydrate. The compounds were characterized by spectroscopic methods. X-ray crystal structure determination and DFT calculations confirmed their geometry in solution and in the solid phase. Moreover, intermolecular interactions in the crystal structure of K2 were analyzed using 3D Hirshfeld surfaces and the related 2D fingerprint plots. The magnetic study revealed very strong antiferromagnetic CuII-CuII exchange interactions, which were supported by magneto-structural correlation and DFT calculations conducted within a broken symmetry (BS) framework. Complexes K1 and K2 exhibited luminescent properties that may be of great importance in the search for new OLEDs. Both K1 and K2 complexes showed emissions in the range of 392–424 nm in solutions at various polarities. Thin materials of the studied compounds were deposited on Si(111) by the spin-coating method or by thermal vapor deposition and studied by scanning electron microscopy (SEM/EDS), atomic force microscopy (AFM), and fluorescence spectroscopy. The thermally deposited K1 and K2 materials showed high fluorescence intensity in the range of 318–531 nm for K1/Si and 326–472 nm for the K2/Si material, indicating that they could be used in optical devices.

A large number of donor atoms, such as O, N, S, P, and supramolecular construction, afford sufficient space for coordination atoms to create mono-, di-, and polynuclear complexes [17][18][19].     decomposition product was a mixture of copper(II) oxide and copper(I) oxide that was additionally confirmed by the XRD analysis ( Figures S6 and S7).     decomposition product was a mixture of copper(II) oxide and copper(I) oxide that was additionally confirmed by the XRD analysis ( Figures S6 and S7).

Crystal Structure Description of [Cu 2 Cl 2 (L)]·H 2 O K2
The structure of the [Cu 2 Cl 2 (L")]·H 2 O K2 (L" = (R)-(+)-1,1 -binaphthalene-2,2 -diamine and 4-tert-butyl-2,6-diformylphenol) complex crystallized in the chiral orthorhombic P2 1 2 1 2 1 space group with all atoms in general positions and the whole molecule given by the formula in the asymmetric unit. Copper(II) cations were found in a pentacoordinated environment with geometrical indices pointing at a very significantly distorted coordination sphere (τ 5 = 0.61 and 0.46 [32] for Cu1 and Cu2, respectively) ( Figure 4). The analysis performed in SHAPE [33] software indicated that Cu1 should rather be described as a trigonal bipyramid (S TBPY = 1.542, S SPY = 3.424), but for Cu2, it did not discriminate unequivocally between the trigonal bipyramid (S TBPY 2.255) and square pyramid (S SPY = 2.236). Both coordination polyhedra shared the common edge due to bridging O22 and O49 oxygen atoms, with Cu1-Cu2 separation (3.090 Å) being even slightly shorter than in K1. Hence, both for K1 and K2 we can expect significant magnetic interactions. The coordination spheres consisted of two nitrogen atoms and two oxygen atoms from the macrocyclic ring and an apical chloride anion. Cu-N bond lengths ranged from 1.951(6) to 2.077(5) Å, Cu-O bonds were from 1.903(5) to 2.045(5) Å, and Cu-Cl were from 2.302(3) to 2.370(2) Å ( Table 2). The naphthyl rings were inclined by 68.1 and 77.5 • for C1/C11 and C28/C38 angles, respectively, whereas the angle between C22a and C49a moieties was 30.0 • . The mutual orientation of these systems imposed the chirality, and the Flack parameter indicated a pure enantiomer.

DC Magnetic Measurements, BS DFT Computations, and EPR Spectra
The MT and M(H) curves for compounds K1 and K2 are presented in Figure 7. At T = 300 K, the MT product for both compounds was close to 0.17 cm 3 K mol -1 , being a value around five times smaller than the 0.867 cm 3 K mol -1 expected for two uncoupled Cu(II) centers assuming gCu = 2.15 within the range typical for 5-coordinative Cu(II) complexes.
With the temperature decreasing to around 100 K, the MT products decreased to reach a 3 -1

DC Magnetic Measurements, BS DFT Computations, and EPR Spectra
The χ M T and M(H) curves for compounds K1 and K2 are presented in Figure 7. At T = 300 K, the χ M T product for both compounds was close to 0.17 cm 3 K mol -1 , being a value around five times smaller than the 0.867 cm 3 K mol -1 expected for two uncoupled Cu(II) centers assuming g Cu = 2.15 within the range typical for 5-coordinative Cu(II) complexes. With the temperature decreasing to around 100 K, the χ M T products decreased to reach a steady value of 0.044 and 0.047 cm 3 K mol -1 for K1 and K2, respectively. Below 10 K, both curves decreased afresh to reach values slightly above 0.040 cm 3 K mol -1 . The shapes of χ M T were interpreted in terms of very strong magnetic exchange coupling between the Cu(II) centers in the Cu 2 O 2 coordination cores through the phenoxo-bridges. The low-temperature part of χ M T, visibly larger than 0, indicated the presence of paramagnetic contribution, which was also confirmed by the M(H) curves.
Sci. 2022, 23, x FOR PEER REVIEW The MT versus T curves were fitted in the 1.8-300 K temperature range u latest PHI software (version 3.1.6, simplex method) [35] and the following Hamil The χ M T versus T curves were fitted in the 1.8-300 K temperature range using the latest PHI software (version 3.1.6, simplex method) [35] and the following Hamiltonian: where only the magnetic exchange constant between Cu(II) centers, J Cu-Cu , and the average g Cu,avg factor for both Cu sites were fitted. The additional magnetic impurities, IMP, were included, employing analytical expression for the temperature-dependent magnetic susceptibility, assuming the mononuclear Cu 2+ complex with g = 2.0. The impurity value represents the fraction of the measured sample K1 or K2, χ = (1-IMP) χ sample + (IMP) χ IMP . The obtained values are presented in Table 3. Table 3. Fitted values of J Cu-Cu , g Cu,avg , and IMP contribution. The J(SUP) a was extracted from the broken symmetry and spin-flip DFT results (for details, see SI section).

Compound K1 K2
J  [36]. Rather a minor difference of around 25 cm -1 between J Cu-Cu values of K1 and K2 (according to the frames of the above correlation) might conveniently be interpreted in terms of minute differences in the Cu-O distances, Cu-O-Cu angles, and torsion angles within the Cu 2 O 2 cores (see crystallographic tables). These results were further nicely supported by the broken symmetry and spin flip DFT computational data (Tables 3 and S1), wherein the J(SUP) [37] values close to −337.0 cm −1 (K1) and −346.5 cm −1 (K2) estimated according to the spin unprojected (SUP) approach, recommended for the strong coupling regime, provided the best illustration of the J Cu-Cu convergence.
The presence of paramagnetic contribution was confirmed by EPR experiments. The powder spectra recorded for K1 and K2 at 77 K, shown in Figure S8, were characteristic for paramagnetic Cu(II) centers. They were successfully simulated with g z = 2.230, g y = 2.072, g x = 2.072, and A z = 177 × 10 −4 cm −1 for K1 and g z = 2.232, g y = 2.091, g x = 2.052, and A z = 173 × 10 −4 cm −1 for K2. The parameters observed for the two complexes were similar and indicated the axial N 2 O 2 coordination environment, which was far less distorted in comparison with dinuclear units, as well as the unpaired electron occupying the molecular orbital with strong contribution from d x2-y2 [38][39][40]. Thus, it is suggested that the paramagnetic contribution was due to the fractional incorporation of the monometallic complex of the Cu II [Cu II vacancy ]L 2 or Cu II Cl[Cu II vacancy ]L(LH) composition in the crystal, represented by the IMP contribution to the simulation of χ M T(T) data. In comparison to the full model Cu II 2 Cl 2 L 2 complex, such a moiety might contain one empty N 2 O 2 pocket, denoted as [Cu vacancy ]. Such a solution relies on the incorporation of around one monometallic complex per eight to nine Cu II 2 Cl 2 L 2 moieties, and is pretty plausible, considering the fact that topological shapes of both moieties are sufficiently similar to each other to accommodate the resultant structural defects without the loss of the crystal stability. The above assumption is supported by the fact that optical inspection of the crystals of K1 and K2 did not indicate the presence of a separate phase, other than the examined crystals. Moreover, crystal structure solution and refinement allow for the presence of some level of such defects without the loss or even with a minute increase in the solution and refinement quality. The presence of paramagnetic "impurities" was previously observed in dinuclear S( 1 / 2 )-S( 1 / 2 ) Cu 2 systems [41][42][43].
The powder EPR spectra of the K1 and K2 complexes recorded at 350 K, at which temperature the S = 1 state is highly populated, showed broad, nearly isotropic lines centered at g eff = 2.14 and 2.13, respectively. The peak-to-peak line widths were about 360 G for K1 and 340 G for K2 ( Figure S9). The broadening of EPR spectra and lack of the resolved g tensor anisotropy were caused by spin-spin interactions between relatively close Cu(II) ions arranged in dimeric units in both complexes. Because the spectra did not undergo the resolution of the signals resulting from the resonance transition between the spin states ∆M S = ±1.0, neither the tensor g components nor the zero-field splitting D parameter can be determined.

UV-VIS and Fluorescence Spectroscopy
The UV-VIS absorption and fluorescence spectra of the copper(II) complexes were recorded at room temperature in solvents of different polarities: chloroform (ε r = 4.9), acetone (ε r = 20.6), methanol (ε r = 32.7), acetonitrile (ε r = 35.9), and DMSO (ε r = 46.5) [44] ( Figure 8, Table S2). Due to the limited solubility of K1 in acetonitrile, we were unable to record the UV-VIS spectrum in MeCN. monometallic complex per eight to nine Cu II 2Cl2L2 moieties, and is pretty plausible, considering the fact that topological shapes of both moieties are sufficiently similar to each other to accommodate the resultant structural defects without the loss of the crystal stability. The above assumption is supported by the fact that optical inspection of the crystals of K1 and K2 did not indicate the presence of a separate phase, other than the examined crystals. Moreover, crystal structure solution and refinement allow for the presence of some level of such defects without the loss or even with a minute increase in the solution and refinement quality. The presence of paramagnetic "impurities" was previously observed in dinuclear S( 1 /2)-S( 1 /2) Cu2 systems [41][42][43].
The powder EPR spectra of the K1 and K2 complexes recorded at 350 K, at which temperature the S = 1 state is highly populated, showed broad, nearly isotropic lines centered at geff = 2.14 and 2.13, respectively. The peak-to-peak line widths were about 360 G for K1 and 340 G for K2 ( Figure S9). The broadening of EPR spectra and lack of the resolved g tensor anisotropy were caused by spin-spin interactions between relatively close Cu(II) ions arranged in dimeric units in both complexes. Because the spectra did not undergo the resolution of the signals resulting from the resonance transition between the spin states ΔMS = ±1.0, neither the tensor g components nor the zero-field splitting D parameter can be determined.

UV-VIS and Fluorescence Spectroscopy
The UV-VIS absorption and fluorescence spectra of the copper(II) complexes were recorded at room temperature in solvents of different polarities: chloroform (εr = 4.9), acetone (εr = 20.6), methanol (εr = 32.7), acetonitrile (εr = 35.9), and DMSO (εr = 46.5) [44] ( Figure 8, Table S2). Due to the limited solubility of K1 in acetonitrile, we were unable to record the UV-VIS spectrum in MeCN. In the UV-VIS spectra of the K1 and K2 complexes, bands in the range of 272-290 nm connected with π → π* transitions in the aromatic rings and the bands from the n → π* transitions of the azomethine group between 322 and 324 nm for K1 and 322 and 328 nm for K2 were recorded. Bands originating from π → π* transitions in the aromatic rings are typical for this kind of compound and were present in the ligand expected range, and thus In the UV-VIS spectra of the K1 and K2 complexes, bands in the range of 272-290 nm connected with π → π* transitions in the aromatic rings and the bands from the n → π* transitions of the azomethine group between 322 and 324 nm for K1 and 322 and 328 nm for K2 were recorded. Bands originating from π → π* transitions in the aromatic rings are typical for this kind of compound and were present in the ligand expected range, and thus we do not show them in Figure 7; only the bands from the charge transfer and d-d transitions are shown.
Band maxima related to the ligand-to-metal charge transfer transition (LMCT) were observed in the range of 388 -408 nm in a solvent at different polarity: methanol (388 nm), DMSO (398 nm), acetone (402 nm), and chloroform (408 nm) for K1, and methanol (388 nm), acetonitrile (392 nm), DMSO (394 nm), acetone (400 nm), and chloroform (404 nm) for K2 [30]. For both compounds, the bathochromic shift of the LMCT band with a decrease in the solvent polarity (except methanol) was noted ( Figure 8, Table S2). This can be connected with the polar character of methanol, which is a protic solvent and causes a different type of interaction with compounds in comparison with the rest of the aprotic solvents [32,45]. Moreover, this can also originate from the distortion of the molecule geometry in the excited state, which implies an increase in the resonance energy and bathochromic shifts.
Additionally, in the absorption spectra, the presence of low-intensity bands at 660 nm for K1 and 664 nm for K2 absorption bands from d-d transitions [46] only in the less polar solvent chloroform were noted. This results from the square pyramidal or trigonal bipyramid environment of the copper atoms shifted towards the apical chloride anion [23,47]. The same was observed previously for similar copper(II) compounds [41,48].
Furthermore, the UV-VIS spectra of the compounds were also registered at room temperature in the solid state ( Figure 9). The spectra show band maxima in the range of 265-266 nm related to π → π* transitions of the aromatic groups and between 385 and 387 nm related to n → π* transitions of the azomethine groups. Moreover, at 468 nm and 461 nm, bands connected with the ligand-to-metal charge transfer LMCT π → d transitions were observed. Above 700 nm for K1 and 720 nm for K2, bands from d-d transitions appeared. The band maxima were shifted towards higher wavelengths by 57-80 nm (LMCT π → d), 63-65 nm (n → π* C=N ), and 40-56 nm (d-d) in comparison to the solvents. This shift is connected to the increase in the rigidity of the complexes' structures in the solid state in comparison to the solution. A red shift of the bands was noted in the spectra of other copper(II) complexes [49].
DMSO (398 nm), acetone (402 nm), and chloroform (408 nm) for K1, and methanol (388 nm), acetonitrile (392 nm), DMSO (394 nm), acetone (400 nm), and chloroform (404 nm) for K2 [30]. For both compounds, the bathochromic shift of the LMCT band with a decrease in the solvent polarity (except methanol) was noted ( Figure 8, Table S2). This can be connected with the polar character of methanol, which is a protic solvent and causes a different type of interaction with compounds in comparison with the rest of the aprotic solvents [32,45]. Moreover, this can also originate from the distortion of the molecule geometry in the excited state, which implies an increase in the resonance energy and bathochromic shifts.
Additionally, in the absorption spectra, the presence of low-intensity bands at 660 nm for K1 and 664 nm for K2 absorption bands from d-d transitions [46] only in the less polar solvent chloroform were noted. This results from the square pyramidal or trigonal bipyramid environment of the copper atoms shifted towards the apical chloride anion [23,47]. The same was observed previously for similar copper(II) compounds [41,48].
Furthermore, the UV-VIS spectra of the compounds were also registered at room temperature in the solid state ( Figure 9). The spectra show band maxima in the range of 265-266 nm related to π → π* transitions of the aromatic groups and between 385 and 387 nm related to n → π* transitions of the azomethine groups. Moreover, at 468 nm and 461 nm, bands connected with the ligand-to-metal charge transfer LMCT π → d transitions were observed. Above 700 nm for K1 and 720 nm for K2, bands from d-d transitions appeared. The band maxima were shifted towards higher wavelengths by 57-80 nm (LMCT π → d), 63-65 nm (n → π*C=N), and 40-56 nm (d-d) in comparison to the solvents. This shift is connected to the increase in the rigidity of the complexes' structures in the solid state in comparison to the solution. A red shift of the bands was noted in the spectra of other copper(II) complexes [49].

Emission Studies
The excitation of K1 and K2 in all solvents at 350 nm resulted in blue emission between 398 and 424 nm for K1 and 392 and 424 nm for K2 ( Figure 10). Emission band maxima of K1 and K2 exhibited bathochromic shifts with increasing solvent polarity. Moreover, the highest fluorescence intensity in most polar solvents such as DMSO and methanol was noted ( Figure 10, Table S2). A similar situation also occurred in the case of other metal(II) complexes [23]. When the emission spectra registered in a solution and in the solid state were compared, it was possible to infer that the solvent destroyed the π-π interactions, and thus the transition energy was increased in the solution, as was observed previously [50].

Emission Studies
The excitation of K1 and K2 in all solvents at 350 nm resulted in blue emission between 398 and 424 nm for K1 and 392 and 424 nm for K2 ( Figure 10). Emission band maxima of K1 and K2 exhibited bathochromic shifts with increasing solvent polarity. Moreover, the highest fluorescence intensity in most polar solvents such as DMSO and methanol was noted ( Figure 10, Table S2). A similar situation also occurred in the case of other metal(II) complexes [23]. When the emission spectra registered in a solution and in the solid state were compared, it was possible to infer that the solvent destroyed the π-π interactions, and thus the transition energy was increased in the solution, as was observed previously [50].

Circular Dichroism
The chiral character of the studied complexes is reflected in their CD spectra ( Figure 11).

Circular Dichroism
The chiral character of the studied complexes is reflected in their CD spectra ( Figure 11).

Circular Dichroism
The chiral character of the studied complexes is reflected in their CD spectra (F Figure 11. CD spectra of K1 and K2 in chloroform 1 × 10 −4 M. The two studied complexes had similar CD spectra with the signals at 314 and 365 nm(−198) for K1, and at 311 nm (+18) and 358 nm (−198) for K2. The Cott noted above 400 nm at 406(+200) and 444(−174) for K1, and at 403(+198) and 440( K2 were connected with n → π*C=N transitions. Conversely, the bands observed a for K1 and 584 nm for K2 from d-d transitions in Cu ions were a result of a square-pyramidal or trigonal pyramidal geometry [24,51]. The low inten corresponding to the d-d transitions largely exhibited the same position (≈585 even a similar intensity for both complexes. This feature can be explained by the e of an identical {CuN2O2Cl} chromophore. The replacement of a tert-butyl grou methyl group in the ring did not affect the optical activity of the complexes, whi consequence of the similarity of the geometry of the studied compounds [52]. M the signs of the CD bands in the spectra of both complexes K1 and K2 were t because they were derivatives of the same enantiomer of diamine ((R binaphthalene-2,2′-diamine) [52,53], as was observed for a series of copper(II) co with chiral tri-and tetradentate Schiff base ligands derived from 1,1'-binaph diamine [14]. for K2 were connected with n → π* C=N transitions. Conversely, the bands observed at 589 nm for K1 and 584 nm for K2 from d-d transitions in Cu ions were a result of a distorted square-pyramidal or trigonal pyramidal geometry [24,51]. The low intense band corresponding to the d-d transitions largely exhibited the same position (≈585 nm) and even a similar intensity for both complexes. This feature can be explained by the existence of an identical {CuN 2 O 2 Cl} chromophore. The replacement of a tert-butyl group with a methyl group in the ring did not affect the optical activity of the complexes, which was a consequence of the similarity of the geometry of the studied compounds [52]. Moreover, the signs of the CD bands in the spectra of both complexes K1 and K2 were the same because they were derivatives of the same enantiomer of diamine ((R)-(+)-1,1 -binaphthalene-2,2diamine) [52,53], as was observed for a series of copper(II) complexes with chiral tri-and tetradentate Schiff base ligands derived from 1,1'-binaphthyl-2,2'-diamine [14].

Theoretical Calculations
The vertical absorption spectrum estimated within the ωB97X-D/def2-SVP/PCM(CHCl 3 ) approach exhibited small intensity signals above 640 nm, corresponding to the d-d* transition forbidden by the Laporte rule (see Figure 12 and the corresponding natural transition orbitals in Figure 13a). The band of about 480 nm involved the transition between the metal and the ligand (the corresponding natural orbitals are presented in Figure 13b). The signals appearing below 400 nm solely arose from the π→π * excitations in the ligand. The shape of the spectrum was only mildly affected by the change of the substituent in the ligand macrocyclic ring from methyl in K1 to tert-butyl in K2. The computational results confirmed the assignment provided above on the basis of the experimental measurements in solution.
corresponding natural transition orbitals in Figure 13a). The band of about 480 n involved the transition between the metal and the ligand (the corresponding natur orbitals are presented in Figure 13b). The signals appearing below 400 nm solely aro from the π→π * excitations in the ligand. The shape of the spectrum was only mild affected by the change of the substituent in the ligand macrocyclic ring from methyl in K to tert-butyl in K2. The computational results confirmed the assignment provided abo on the basis of the experimental measurements in solution.

Thin Materials of Copper(II) Complexes
The morphology and roughness of the thin layers were examined by SEM and AFM techniques. To test the chemical composition of materials, the EDS analysis was recorded (Figures 14d, 15, 16, S10 and S11). The optimal parameters of the layers (roughness, parameters, and homogeneity) were obtained in a multi-stage centrifugation spin-coated process using particular parameters: 2500 rpm to 3000 rpm, time of coating 5 or 10 s. Moreover, the thermal vapor deposition method was also used as a second technique to achieve thin materials. The two-dimensional (2D) and three-dimensional (3D) AFM images scanned over a surface area of 1 × 1 μm 2 are shown in Figures 14, 17 and S12. The values of

Thin Materials of Copper(II) Complexes
The morphology and roughness of the thin layers were examined by SEM and AFM techniques. To test the chemical composition of materials, the EDS analysis was recorded (Figures 14d, 15, 16, S10 and S11). The optimal parameters of the layers (roughness, parameters, and homogeneity) were obtained in a multi-stage centrifugation spin-coated process using particular parameters: 2500 rpm to 3000 rpm, time of coating 5 or 10 s. Moreover, the thermal vapor deposition method was also used as a second technique to achieve thin materials. The two-dimensional (2D) and three-dimensional (3D) AFM images scanned over a surface area of 1 × 1 µm 2 are shown in Figures 14, 17 and S12. The values of roughness parameters of materials obtained by thermal deposition were as follows: K1/Si R a = 10.7-13.1 nm and R q = 13.2-17.1 nm, and K2/Si R a = 3.91-4.96 nm and R q = 4.02-6.38 nm. The roughness of the spin-coated films was similar to that obtained by thermal deposition. However, the spin-coated materials were thinner than those achieved by thermal vapor deposition. A similar situation was noted by us in the case of the layers L1/Si or L2/Si of the macrocyclic Schiff bases derived from ophenylenediamine and 2-hydroxy-5-methylisophthalaldehyde L1 or 2-hydroxy-5-tert-butyl-1,3-benzenedicarboxaldehyde L2 [54].  The new films obtained by thermal vapor deposition were also characterized by IR DRIFT ( Figure S13). The analysis of the IR DRIFT data showed the presence of the characteristic for the Schiff base peaks between 1653 and 1647 cm −1 from stretching frequencies of the azomethine group, and bands from stretching vibrations of aromatic rings νC=CAr in the region 1568-1485 cm −1 were registered. The above-described bands confirmed the presence of the deposited compounds in the obtained materials.

Fluorescence Properties of the Materials
The fluorescence properties of the thin materials were also studied. The height (thickness) of the spin-coated materials was less than half that of thermally deposited films (70 nm K1/Si and 24 nm K2/Si), which influenced the emission properties of the composites. The spincoated K1/Si materials did not exhibit fluorescence. Conversely, in the case of K2/Si film (Figure 18), the high intensity of the emission bands (λex = 320 nm) was observed.  The values of the roughness parameters for thin materials obtained by both spincoating and by thermal vapor deposition indicate the achievement of smooth, thin films of copper(II) complexes. Moreover, SEM/EDS analysis showed the presence of carbon, nitrogen, oxygen, and copper in the layer (Figures S10 and S11). SEM/EDS, together with mapping analysis, confirmed the composition of the new materials.
The new films obtained by thermal vapor deposition were also characterized by IR DRIFT ( Figure S13). The analysis of the IR DRIFT data showed the presence of the characteristic for the Schiff base peaks between 1653 and 1647 cm −1 from stretching frequencies of the azomethine group, and bands from stretching vibrations of aromatic rings ν C=CAr in the region 1568-1485 cm −1 were registered. The above-described bands confirmed the presence of the deposited compounds in the obtained materials.

Fluorescence Properties of the Materials
The fluorescence properties of the thin materials were also studied. The height (thickness) of the spin-coated materials was less than half that of thermally deposited films (70 nm K1/Si and 24 nm K2/Si), which influenced the emission properties of the composites. The spin-coated K1/Si materials did not exhibit fluorescence. Conversely, in the case of K2/Si film (Figure 18), the high intensity of the emission bands (λ ex = 320 nm) was observed.
The thin thermally deposited materials showed fluorescence in the range of 318-531 nm for K1/Si and 326-472 nm for the K2 material, λ ex = 250 nm. Furthermore, the emission bands were broad and split into three components ( Figure 19, Table S3). The highest intensity of the emission bands for the smooth, thin layer with the equally distributed complexes on the Si surface was noted (Figures 18 and 19). The bathochromic shift of the emission bands of the films in comparison to the solutions was noted. Red shifting of emission maxima was observed for most fluorescent compounds in the solid state, probably due to π-π stacking of the aromatic rings in the molecules [49,54]. An influence of molecular packing in the solid phase on the optical properties can therefore be concluded. This can arise from a different pathway of non-radiative transitions. It can be related to the reduction of the ligand conformational flexibility in the complex. This reduction results from the restraints imposed by the substrate surface. Layers obtained by thermal deposition methods are intended to be used as optical materials.
rings νC=CAr in the region 1568-1485 cm −1 were registered. The above-described ban confirmed the presence of the deposited compounds in the obtained materials.

Fluorescence Properties of the Materials
The fluorescence properties of the thin materials were also studied. The height (thickne of the spin-coated materials was less than half that of thermally deposited films (70 nm K1 and 24 nm K2/Si), which influenced the emission properties of the composites. The sp coated K1/Si materials did not exhibit fluorescence. Conversely, in the case of K2/Si f (Figure 18), the high intensity of the emission bands (λex = 320 nm) was observed. The thin thermally deposited materials showed fluorescence in the range of 318-5 nm for K1/Si and 326-472 nm for the K2 material, λex = 250 nm. Furthermore, the emiss bands were broad and split into three components ( Figure 19, Table S3). The high intensity of the emission bands for the smooth, thin layer with the equally distribu complexes on the Si surface was noted (Figures 18 and 19). The bathochromic shift of emission bands of the films in comparison to the solutions was noted. Red shifting emission maxima was observed for most fluorescent compounds in the solid sta probably due to π-π stacking of the aromatic rings in the molecules [49,54]. An influen of molecular packing in the solid phase on the optical properties can therefore concluded. This can arise from a different pathway of non-radiative transitions. It can

XAS Analysis
The normalized spectra of K1 and K2 were very similar due to the stru similarity of copper coordination spheres in both complexes. Those spectra showe features for L3 and another two for the L2 edge ( Figure 20, Table 4). In the case of edge, they occurred at 931.0 and 934.8 eV for K1 and 931.0 and 934.7 eV for K2, and features were shifted by around 20 eV towards higher energies. Those values common for Cu(II) compounds [55][56][57]. According to the theory, the intensity of L3 was around twofold stronger than in the case of L2, and only one peak related to 2p transitions was expected [58][59][60]. However, additional features are very often obs due to 2p4s transitions [61][62][63]. Those additional peaks are usually around 25 weaker due to the smaller cross-section for such X-ray absorption. DeBeer George showed for copper dimers with macrocyclic thiolate ligands and copper ions sepa by around 2.9 Å that the L energy pattern depends on the effective nuclear charg ligand field splitting and also possible metal-metal bonding [64]. Muzioł et al. sugg also that a more complex pattern of the L edge might result from strongly dist coordination spheres [56]. In the reported structures, we observed such a deformatio Section 2.2.), and the Cu-Cu distance was around 3.1 Å. Hence, we observed much w signals following the main features of the L3 and L2 edges.

XAS Analysis
The normalized spectra of K1 and K2 were very similar due to the structural similarity of copper coordination spheres in both complexes. Those spectra showed two features for L 3 and another two for the L 2 edge (Figure 20, Table 4). In the case of the L 3 edge, they occurred at 931.0 and 934.8 eV for K1 and 931.0 and 934.7 eV for K2, and the L 2 features were shifted by around 20 eV towards higher energies. Those values were common for Cu(II) compounds [55][56][57]. According to the theory, the intensity of L 3 peaks was around twofold stronger than in the case of L 2 , and only one peak related to 2p→3d transitions was expected [58][59][60]. However, additional features are very often observed due to 2p→4s transitions [61][62][63]. Those additional peaks are usually around 25 times weaker due to the smaller cross-section for such X-ray absorption. DeBeer George et al. showed for copper dimers with macrocyclic thiolate ligands and copper ions separated by around 2.9 Å that the L energy pattern depends on the effective nuclear charge the ligand field splitting and also possible metal-metal bonding [64]. Muzioł et al. suggested also that a more complex pattern of the L edge might result from strongly distorted coordination spheres [56]. In the reported structures, we observed such a deformation (see Section 2.2), and the Cu-Cu distance was around 3.1 Å. Hence, we observed much weaker signals following the main features of the L 3 and L 2 edges. weaker due to the smaller cross-section for such X-ray absorption. DeBeer George et al. showed for copper dimers with macrocyclic thiolate ligands and copper ions separated by around 2.9 Å that the L energy pattern depends on the effective nuclear charge the ligand field splitting and also possible metal-metal bonding [64]. Muzioł et al. suggested also that a more complex pattern of the L edge might result from strongly distorted coordination spheres [56]. In the reported structures, we observed such a deformation (see Section 2.2.), and the Cu-Cu distance was around 3.1 Å. Hence, we observed much weaker signals following the main features of the L3 and L2 edges. Figure 20. Normalized XANES spectra of copper L2,3-edge with peaks corresponding to 2p 6 3d 9  2p 5 3d 10 . The signal for K1 was shifted by 2 to separate both spectra. Figure 20. Normalized XANES spectra of copper L 2,3 -edge with peaks corresponding to 2p 6 3d 9 → 2p 5 3d 10 . The signal for K1 was shifted by 2 to separate both spectra. Table 4. Summary of spectral features of the Cu absorption at the L-edges (peak energies and intensities).

Methods and Instrumentation
UV-VIS absorption spectra were recorded in chloroform, acetone, DMSO, acetonitrile, and methanol (3.323 × 10 −6 M) solutions on a Hitachi spectrophotometer. The fluorescence spectra were recorded on a spectrofluorometer Gildenpλotonics 700 (Dublin, Ireland) in the range 900-200 nm (grating 1, bandpass 5 and 8, integration time 100 ms, chloroform, acetone, DMSO, acetonitrile, and methanol solution of compounds the same as in the case of the UV-VIS studies or silicon slides). The elemental analysis was carried out using a Vario EL III Elemental analyzer. The thermal analysis (TG, DTG, DTA) was performed on an SDT 2960 TA analyzer under air, a heating rate of 10 • C min −1 , and a heating range of up to 1000 • C and a Jupiter STA 449 F5 thermoanalyzer from Netzsch (Selb, Germany) with an automatic sample feeder coupled to a Vertex 70V FT-IR spectrometer from Bruker Optik (Ettlingen, Germany). After combustion, the residue of the sample was analyzed by an XRD analysis performed with a Philips X'Pert equipped with an X'Celerator Scientific detector. The IR spectra were recorded on the Bruker instrument using the ATR technique in the range of 70-4000 cm −1 . Circular dichroism spectra were recorded with a Jasco J-815 spectropolarimeter (Jasco Inc.) in the range of 310-700 nm wavelengths. The solution of K1 and K2 complexes (≈1 × 10 −4 M) was prepared by dissolving it in a CHCl 3 solution.

Spin Coating
Layers of the complexes were deposited on Si(111) wafers (10 nm × 10 mm) that were ≈500 nm thick using the spin coating technique. Precursors were dissolved in chloroform and deposited on Si using a spin coater (Laurell 650 SZ). The spin speed varied from 2500 to 3000 rpm, and the coating time was 5 or 10 s.

Thermal Vapor Deposition
The thin layer of K1 and K2 was deposited on n-type silicon substrate. The orientation of the silicon substrate was (100) with electrical resistivity (ρ) equal to 6.2 × 10 −3 Ω cm. The silicon wafer was first degreased in acetone, ethanol, and finally in deionized water using an ultrasonic bath. On the front side (polished side) of the silicon wafer, a K1 and K2 layers of 24-70 nm thickness were deposited in a vacuum (p = 2 × 10 −4 Pa) by a thermal evaporation method, with an evaporation rate of 0.2 nm/s, without heating of the substrate.
The morphology and composition of the obtained films were analyzed with a scanning electron microscope (SEM; LEO Electron Microscopy Ltd, Cambridge, UK), the 21430 VP model equipped with secondary electrons (SE) detectors, and an energy-dispersive X-ray spectrometer (EDX) Quantax with an XFlash 4010 detector (Bruker AXS microanalysis GmbH, Berlin, Germany). The atomic force microscopy (AFM) images were performed in the tapping mode with a Multi Mode Nano Scope IIIa (Veeco Digital Instrument, SB, US) microscope. The structure of the produced layers was estimated using diffuse reflectance infrared Fourier transform spectroscopy (DRIFT, Spectrum 2000, PerkinElmer Inc., Waltham, MA, USA). The absorption spectra of the solid samples K1 and K2 were recorded on the Jasco V-750 spectrophotometer in the 200-800 nm (bandwidth 1.0 nm, data interval 0.2 nm).

Crystal Structure Determination
The diffraction data of the studied compounds were collected for the single crystal at 100 K using an XtaLAB Synergy Dualflex equipped with a HyPix detector and CuK α source (λ = 1.54184 Å) for K1 and on BL14.2 beamline (Helmholtz Zentrum Berlin, Bessy II) operating at λ = 0.7999 Å for K2. For K1, the full process of the data reduction was performed in CrysAlis Pro [65], whereas for K2, the data reduction and space group determination were performed with xdsapp [66,67], and then CrysAlis Pro was used for final data reduction. For K2, the absorption correction was introduced by the diffabs method implemented into WinGx [68]. The structure was solved by the direct methods and refined with the full-matrix least-squares procedure on F 2 (SHELXL-2018/1) [69]. All heavy atoms were refined with anisotropic displacement parameters. Hydrogen atoms were located at calculated positions with thermal displacement parameters fixed to a value of 20% or 50% higher than those of the corresponding carbon atoms. It should be noted that for K1, the bypass procedure implemented into Olex2 [34] was applied due to poorly defined density in the solvent region of the porous complex. It resulted in significant amelioration of the final model. However, the whole interaction model suffered from missing solvent-complex and solvent-solvent interactions. In K2, the O81 water molecule was refined with partial occupancy (0.5), and the O21 molecule was located very close to the inversion center. In the final model of K2, there were missing hydrogen atoms from the O81 water molecule. The stable refinement was achieved with ISOR and DELU restraints for the positionally disordered C(61)H 3 methyl group in K1 and for (ISOR) for C62, C64, and C74 atoms from tert-butyl groups of K2. All figures were prepared in DIAMOND [70] and ORTEP-3 [71]. The results of the data collection and refinement are summarized in Table 5.

SQUID Measurements
Magnetic measurements were investigated using a Quantum Design MPMS 3 SQUID magnetometer. For the measurements, powdered compounds K1 and K2 were sealed in two foil bags. The dc magnetic susceptibilities were measured in the 300-1.8K temperature range with an applied field of 5 kOe. The measurements were carried out in sweep mode with a scan rate of 2 K min -1 . The magnetization curves were measured in the 0-70 kOe range with dc field stabilization. Magnetic data were corrected for the diamagnetic contribution of the plastic bags and sample by empirical and Pascal's constants, respectively [72]. Moreover, the TIP contribution of 5.9 × 10 −5 cm 3 mol −1 for Cu(II) metal ion was applied.

EPR Measurements
EPR experiments were carried out for powder samples using a Bruker Elexsys E500 spectrometer operating at ∼9.6 GHz (X-band) frequency. The spectrometer was equipped with an NMR teslameter and a frequency counter. The temperature was controlled by using a finger-Dewar for measurements at 77 K and a Bruker ER 4131VT variable temperature accessory for 350 K. We set the amplitude and frequency of the modulating field to 10 G and 100 kHz, respectively, and we set the microwave power to 20 mW. The EPR spectra were simulated using EasySpin 5.2.35 [73,74].

Theoretical Calculations
The full geometry optimization of K1 and K2 was performed within the ωB97X-D/def2-SVP approach in a vacuum for magnetic coupling analysis and in the PCM model of chloroform for photophysical properties, starting from the crystal structure. The character of the stationary points was confirmed with the harmonic vibration analysis. Vertical absorption was investigated within the same approach, and ECD spectra were depicted for the analyzed enantiomers. The corresponding natural transition orbitals were examined in order to determine the character of the most intensive transitions. All these calculations were carried out with the Gaussian16 program [75]. The magnetic coupling parameters of the complexes were estimated within the broken symmetry approach and spin-flip formalism in B3LYP functional, according to the recommendations of Neese et al. [76] for the gas phase optimized geometry of both complexes. Moreover, the moderate-size def2-SVP basis set was applied for these calculations for the light atoms, as it has been proven to provide a good cost-to-quality balance for large systems containing copper atoms, and the basis set for copper was extended to the def2-QZVPP one [76]. Moreover, the spin-flip formalism was also employed with the same functional and basis set, for comparison. The magnetic coupling constants J were estimated according to spin-unprojected (SUP) scheme proposed by Ruiz for the strong coupling regime [37,77]. The corresponding calculations are based on the total spin-coupling Hamiltonian of the form -2J(Cu 1 -Cu 2 )S Cu1 S Cu2 , where J(Cu 1 -Cu 2 ) is the exchange coupling constant between the two copper atoms with total spins S Cu1 and S Cu2 , individually. Additionally, the spin-projected scheme and approximated spin-projected scheme were also applied for comparison, and the corresponding data are presented in the Supporting Information. All the magnetic coupling constant calculations were carried out with the Orca program package [78].

XAS
X-ray absorption spectra were recorded at the National Synchrotron Radiation Centre SOLARIS at the bending magnet PIRX beamline equipped with a collimated Plane Grating Monochromator for a copper L2,3-edge (910-1040 eV). The sample was finely ground and attached to double-sided adhesive conductive graphite tape. The measurements were performed with the step size of 0.25 eV for the pre-edge region, 0.15 eV for the edge regions, and 0.5 eV for the high energy part. The data sets were collected at room temperature in an ultra-high vacuum (UHV) using total electron yield mode (TEY). The data were processed using the ATHENA program from the Demeter package [79].

K2
A total of 0.5 mmol of 4-tert-butyl-2,6-diformylphenol, 0.5 mmol of (R)-(+)-1,1 -binaphthalene-2,2 -diamine, 0.5 mmol of copper(II) chloride dihydrate, and excess of triethylamine were dissolved in 80 cm 3 of methanol. The synthesis was carried out under reflux for 1 hour. The product was dried under air, and single brown crystals were crystalized in slow evaporation using a mixture of acetonitrile/chloroform and determined by crystal analysis.  Figure S2).

Conclusions
The research presented herein describes the synthesis of two new macrocyclic dinuclear copper(II) complexes, with N 4 O 2 donor atoms. The Cu(II) complexes K1 and K2 were prepared by the template reaction of (R)-(+)-1,1 -binaphthalene-2,2 -diamine and 2-hydroxy-5-methyl-1,3-benzenedicarboxaldehyde K1, or 4-tert-butyl-2,6-diformylphenol K2 with copper(II) chloride dihydrate. The X-ray data show that copper(II) cations are in a heavily distorted pentacoordinated environment. The coordination spheres consist of two nitrogen atoms and two oxygen atoms from the macrocyclic ring and apical chloride anion. In the case of K1, the voids accounting for 1231.5 Å 3 (22.7% of the volume cell) were noted, whereas for K2, channels running along the b axis accounted for 461.2 Å3 (8.3% of the cell volume) filled with water molecules forming C52-H52 . . . O81[1-x, -1/2+y, 1/2-z] hydrogen bonds existed. The magnetic studies showed very strong antiferromagnetic Cu II -C II exchange interactions represented by J Cu-Cu = −305.66 ± 0.05 cm −1 for K1 and J Cu-Cu = −328.45 ± 0.16 cm −1 for K2, which were nicely correlated with structural data and confirmed by the broken symmetry DFT calculations. The EPR spectra of the complexes K1 and K2 showed broad, nearly isotropic lines centered at g eff = 2.14 and 2.13, respectively. The broadening of EPR spectra and lack of the resolved g tensor anisotropy were caused by spin-spin interactions between relatively close Cu(II) ions arranged in dimeric units in both complexes. The compliance between experimental and theoretical results validated the developed calculation method, which will be used to design new binuclear copper(II) complexes. The obtained complexes exhibited emission in the various polarity solvents and in the solid state. The blue emission between 398 and 424 nm for K1 and 392 and 424 nm for K2 in a solvent at different polarities was observed. The bathochromic shift with increasing solvent polarity for K2 was also observed. The highly ordered materials were obtained by spin-coating and thermal vapor methods, exhibiting fluorescence in the range of 318-531 nm for K1/Si and 326-472 nm for the K2/Si material, λ ex = 250 nm (thermally deposited films). The emission bands were broad and split into three components. The bathochromic shift of the fluorescence bands of films in comparison to that of the solution was noted. This can result from molecular packing in the solid state being different to that in the solution. The fluorescence emission of the layers makes these films potentially suitable for application in light-emitting devices.