Supporting Information. A Hemispherand-Strapped Calix[4]pyrrole: An Ion-pair. Receptor for the Recognition and Extraction of Lithium Nitrite
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1 Supporting Information For A Hemispherand-Strapped Calix[4]pyrrole: An Ion-pair Receptor for the Recognition and Extraction of Lithium Nitrite Qing He, Zhan Zhang, James T. Brewster, Vincent M. Lynch, Sung Kuk Kim *, and Jonathan L. Sessler * Department of Chemistry, The University of Texas at Austin, 105 East 24th, Street-Stop A5300, Austin, Texas , United States Institute for Supramolecular and Catalytic Chemistry, Shanghai University, 99 Shangda Road, Shanghai , China Department of Chemistry and Research Institute of National Science, Gyeongsang National University, Jinju, , Korea * Corresponding author: Jonathan L. Sessler ( sessler@mail.utexas.edu), Sung Kuk Kim ( sungkukkim@gnu.ac.kr) 1. General Information 2. Synthesis 3. Crystal structure of 1 LiCl Contents 4. 1 H NMR spectroscopic titrations of receptor 1 with LiClO4 or NaClO4 5. DFT calculations 6. 1 H NMR spectral titrations used to determine binding constants 7. Proposed LiNO2 complexation pathways for 1 8. X-ray Experimental 9. References 10. Energies and geometrical coordinates of the optimized models in the gas phase 11. Additional high resolution mass spectra and NMR spectra S1
2 1. General Information All solvents and chemicals used were purchased from Aldrich, TCI, and Acros and used without further purification. TLC analyses were carried out by using Sorbent Technologies silica gel (200 mm) sheets. Column chromatography was performed on Sorbent silica gel 60 (40 63 mm). NMR spectra were recorded on a Varian Mercury 400 instrument. The NMR spectra were referenced to solvent residue peaks and the spectroscopic solvents were purchased from Cambridge Isotope Laboratories and Aldrich. Electrospray ionization (ESI) mass spectra were recorded on a VG AutoSpec apparatus. X-ray crystallographic analyses were carried out on either a Rigaku AFC12 diffractometer equipped with a Saturn 724+ CCD or an Agilent Technologies SuperNova Dual Source diffractometer using a µ-focus Cu Kα radiation source (λ = Å) with collimating mirror monochromators. A graphite monochromator and MoKα radiation were used. Further details of the structures and their refinement is given in a later section. 2. Synthesis Scheme S1. Synthesis of intermediate 2. Compounds s1, s3 and s5 were commercially available and s2, s4 were prepared according to literature reports. 1 6, 6'-(2-Methoxy-1, 3-phenylene)bis(pyridin-2-amine) (2) Compounds s4 (1.80 g, 5mmol), s5 (1.73 g, 10 mmol), Pd(PPh 3) 4 (346 mg, 0.3 mmol), and K 3PO 4 (6.36 g, 30 mmol) were mixed and dissolved in dry DMF (60 ml) and then heated to 110 under an N 2 atmosphere and then stirred for 5 h. After allowing the reaction mixture to cool to room temperature, the mixture was diluted with ethyl acetate (150 ml). The resulting solution was washed with water (5 60 ml). The combined organic phase was dried over anhydrous Na 2SO 4 for 4 h. After evaporation of the solvent, the residue was subjected to flash column over silica gel eluting with dichloromethane/methanol/triethylamine (100:4:1) to obtain the products (0.92 g, 63%) as an off-white solid. 1 H NMR (400 MHz, CD 3OD): δ (m, 4H, ArH), (t, J = 8.0 Hz, 1H, ArH), (dd, J = 8.0 Hz, 0.8 Hz, 2H, ArH), (dd, J = 8.0 Hz, 0.8 Hz, 2H, ArH), 3.33 (s, 3H, OMe); 13 C NMR (100 MHz, CD 3OD): δ 160.8, 157.0, 155.5, 139.3, 136.0, 132.2, 124.9, 115.0, 108.6, 61.8; HRMS (ESI) m/z [M + H] + calcd for C 17H 17N 4O, found S2
3 Scheme S2. Synthesis of intermediate 3. 4, 4-Di(1H-pyrrol-2-yl)pentanoic acid (3): A mixture of levulinic acid s6 (30.01 g, 259 mmol) and pyrroles s7 (80.05 g, excess) were dissolved in Et 2O (400 ml). Methanesulfonic acid (1.5 ml) was added dropwise, then stirred at room temperature overnight. The mixture was washed with water (8 200 ml) and the organic phase was separated and dried over anhydrous Na 2SO 4. The solvent was removed under reduced pressure and the resulting residue was subjected to flash column over silica gel using dichloromethane (DCM) as the eluent, obtaining the product 3 as white solid (11.48 g, 19%). 1 H NMR (400 MHz, CD 3OD): δ 9.66 (brs., 2H, NH), (m, 2H, pyrrole-h), (m, 2H, pyrrole-h), (m, 2H, pyrrole-h), (m, 2H, CH 2), (m, 2H, CH 2), 1.57 (s, 3H, CH 3); 13 C NMR (100 MHz, CD 3OD): δ 178.9, 139.7, 118.9, 108.6, 106.2, 40.7, 38.2, 31.8, 27.3; HRMS (ESI) m/z [M + Na] + calcd for C 13H 16N 2NaO 2, found Synthesis of precursor 4: To a mixture of compound 2 (1.15 g, 3.9 mmol), 3 (2.26 g, 9.7 mmol), and EDCI HCl (2.50 g, 13.0 mmol) in DCM (120 ml) 5 ml of pyridine was added. The resulting solution was stirred at room temperature under an N 2 atmosphere for 36 h. After the DCM was removed under reduced pressure, the residue was subjected to silica gel column eluting with ethyl acetate/hexanes (1/3, v/v) to give 2.31 g (81% yield) of 4 as thick oil (s, 2H, CONH), (m, 6H), 7.76 (t, J = 8.0 Hz, 2H, ArH), (d, J = 8.0 Hz, 2H, ArH), (dd, J = 8.0 Hz, 4.0 Hz, 1H, ArH), (m, 4H, pyrrole-h), (m, 8H, pyrrole-h), 3.27 (s, 3H, OMe), (m, 4H, CH 2), (m, 4H, CH 2), 1.57 (s, 6H, CH 3); 13 C NMR (100 MHz, CD 2Cl 2): δ 173.0, 157.3, 155.6, 152.3, 139.7, 138.3, 134.9, 132.8, 125.3, 121.6, 118.4, 113.3, 108.9, 106.0, 62.6, 39.9, 37.1, 34.3, 27.2; HRMS (ESI) m/z [M + Na] + calcd for C 43H 44N 8NaO 3, found Synthesis of compound 1: BF 3 Et 2O (0.8 ml) was added dropwise to a solution of precursor 4 (2.61 g, 3.6 mmol) in acetone (1000 ml) at RT. The reaction solution was stirred at RT overnight. Then triethylamine (20 ml) was added to quench the reaction. The solvent was removed and the resulting residue was purified by column chromatography over silica gel (eluent: ethyl acetate/hexanes (1/3, v/v)) to give 0.55 g (19% yield) of 1 as an off-white solid. 1 H NMR (400 MHz, CD 2Cl 2): δ (m, 8H), (t, J = 8.0 Hz, 2H, ArH), (d, J = 8.0 Hz, 2H, ArH), (d, J = 8.0 Hz, 2H, ArH), 7.26 (t, J = 8.0 Hz, 1 H, ArH), (m, 8H, pyrrole-h), 3.22 (s, 3H, OMe), (m, 8H, CH 2), (m, 18H, Me); 13 C NMR (100 MHz, CD 2Cl 2): δ 173.3, 157.2, 157.0, 152.0, 140.7, 140.2, 137.8, 135.4, 132.4, S3
4 124.8, 120.1, 113.7, 105.5, 104.5, 62.3, 40.3, 38.2, 36.5, 35.3, 31.7, 29.6, 29.0; HRMS (ESI) m/z [M + Na] + calcd for C 49H 52N 8NaO 3, found Crystal structure of 1 LiCl Figure S1. Single crystal X-ray diffraction structures of compound 1 obtained from the evaporation of solutions of A) acetonitrile; B) a mixture of ethyl acetate and methanol and C) a mixture of chloroform and methanol. Three different structures of 1 were obtained from the analysis of single crystals obtained via the slow evaporation of acetonitrile (A), from a mixture of ethyl acetate and methanol (B), and from a mixture of chloroform, acetonitrile and methanol (C). In all three cases, the calix[4]pyrrole was found to adopt a 1,2-alternate conformation, which differs from that seen for the 0ligoether-strapped calix[4]pyrroles 2 and calix[4]arene-strapped calix[4]pyrroles in the absence of anionic salts. 3 Analysis of Crystal A showed that the cavity formed by the hemispherand was predominantly occupied by a methoxyphenyl group. However, analysis of Crystals B and C revealed the central pockets being occupied by two methanol molecules or two water molecules, respectively. On this basis we inferred that receptor 1 might be sufficiently flexible so as to accommodate lithium salts in the form of ion pairs. S4
5 Figure S2. A) Front view and B) side view of the single crystal X-ray diffraction structure of the lithium complex [1 LiCl H 2O MeOH].This crystal of the complex 1 LiCl H 2O MeOH was obtained by allowing a mixture of receptor 1 and excess lithium chloride, sodium chloride, potassium chloride, and rubidium chloride in CHCl 3/CH 3CN/CH 3OH to undergo slow evaporation. Key metric parameters are: Å for Li1 O1, Å for Li1 N7, Å for Li1 N7, Å for Li1 O2, Å for Li1 N6, and Å for Li1 Cl1, respectively H NMR spectroscopic titrations of receptor 1 with LiClO4 or NaClO4 Figure S3. 1 H NMR titration of receptor 1 with LiClO 4 in a mixed solvent consisting of CD 2Cl 2/CD 3OD (9/1, v/v). The concentration of 1 was 5.0 mm. S5
6 Figure S4. 1 H NMR titration of receptor 1 with NaClO 4 in a mixed solvent consisting of CD 2Cl 2/CD 3OD (9/1, v/v). The concentration of 1 was 5.0 mm. 5. DFT calculations All geometrical optimizations and frequency analyses were carried out with the Gaussian09 suite 4 of programs at the B3LYP/6-31G*//B3LYP/6-31G* level. Frequency analyses were run to confirm that all the structures obtained were local minima. Figure S5. DFT optimized molecular models of the complexes of receptor 1 with (A) LiCl and (B) LiCl H 2O. S6
7 Figure S6. DFT optimized molecular models of the complexes of receptor 1 with (A) NaCl and (B) NaCl H 2O. Figure S7. DFT optimized molecular models of the complexes of receptor 1 with (A) KCl and (B) KCl H 2O. S7
8 Figure S8. DFT optimized molecular models of the complexes of receptor 1 with (A) LiBr; (B) LiNO 2 and (C) LiNO 3. Table S1. Calculated Gas-Phase Binding Distances and Energies for Two Possible Ion Pair Complexes of 1. Table S2. Calculated Gas-Phase Binding Distances and Energy for four Ion Pair complexes of H NMR spectral titrations used to determine binding constants S8
9 Figure S9. Stacked 1 H NMR spectra corresponding to the titration of 1 (5.0 mm) with LiCl (0.9 M) in a mixture of CD 2Cl 2/CD 3OD (9/1, v/v). Figure 10. Binding curve obtained by fitting the chemical shift change of the pyrrole NH signal against [LiCl]. K a = 45 ± 1 M -1.. S9
10 Titration Fitting Curve y =(1+a*K+x*K-sqrt(-4*a*x*K^2+(-1-a*K-x*K)^2))/(2*K)*(dd)/a 0.75 Δδ (ppm) a a K K dd dd Statisti Statisti Value Error Value Error Value Error Reduc Adj. R- deltah C(LiCl)/M Figure S11. Binding curve obtained by fitting the chemical shift change of the pyrrole NH signal against [LiBr]. K a = 74 ± 8 M -1. Titration Fitting Curve 1.50 y =(1+a*K+x*K-sqrt(-4*a*x*K^2+(-1-a*K-x*K)^2))/(2*K)*(dd)/a 1.25 Δδ (ppm) a a K K dd dd Statis Statis Value Error Value Error Value Error Redu Adj. R delta C(LiNO 2 )/M Figure S12. Binding curve obtained by fitting the chemical shift change of the pyrrole NH signal against [LiNO 2]. K a = 108 ± 7 M -1. S10
11 1.5 Titration Fitting Curve y =(1+a*K+x*K-sqrt(-4*a*x*K^2+(-1-a*K-x*K)^2))/(2*K)*(dd)/a Δδ (ppm) a a K K dd dd Statist Statist Value Error Value Error Value Error Reduc Adj. R deltah C(LiNO 3 )/ M Figure S13. Binding curve obtained by fitting the chemical shift change of the pyrrole NH signal against [LiNO 3]. K a = 263 ± 13M -1. Figure S14. 1 H NMR spectroscopic titration of receptor 1 with LiNO 2 in a mixed solvent consisting of CD 2Cl 2/CD 3OD (9/1, v/v). The concentration of 1 was 5.0 mm. S11
12 Figure S15. 1 H NMR titration of receptor 1 with TBANO 2 in a mixture solvent of CD 2Cl 2/CD 3OD (9/1, v/v). The concentration of 1 was 5.0 mm. S12
13 Figure S16. Top: 1 H NMR titration of receptor 1 with lithium tetraphenylborate (LiTPB) in a mixed solvent consisting of CD 2Cl 2/CD 3OD (9/1, v/v). Bottom: 1 H NMR spectroscopic titration of receptor 1 and 20 equiv of LiTBP with TBANO 2 in a mixed solvent system consisting of CD 2Cl 2/CD 3OD (9/1, v/v). The concentration of 1 was 5.0 mm. 7. Proposed LiNO2 complexation pathways for 1 Figure S17. Proposed LiNO 2 complexation pathways for 1. S13
14 8. X-ray Experimental X-ray experimental for the complex of 1 LiCl (right) Single crystals of C54H69ClLiN9O7 [1 LiCl] were obtained as colorless blocks via the slow evaporation of a CHCl3/CH3CN/CH3OH solution of receptor 1 in the presence of excess lithium chloride. A suitable crystal was selected and the data were collected on a Rigaku AFC12 diffractometer with a Saturn 724+ CCD using a graphite. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S18. View of complex of 1 LiCl. Displacement ellipsoids are scaled to the50% probability level. S14
15 Table S3 Crystal data and structure refinement for 1 LiCl Empirical formula C54H69ClLiN9O7 Formula weight Temperature/K Crystal system triclinic Space group P-1 a/å (5) b/å (6) c/å (8) α/ (11) β/ (14) γ/ (11) Volume/Å (2) Z 2 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation MoKα (λ = ) 2Θ range for data collection/ to 62.5 Index ranges -15 h 15, -19 k 18, -25 l 25 Reflections collected Independent reflections [Rint = , Rsigma = ] Data/restraints/parameters 15033/0/693 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-0.68 CCDC Number S15
16 X-ray experimental for the complex of 1 LiCl (left) Single crystals of C54H69ClLiN9O7 [1 LiCl] were obtained as colorless blocks via the slow evaporation of a CHCl3/CH3CN/CH3OH solution of receptor 1 in the presence of excess lithium chloride, sodium chloride, potassium chloride and rubidium chloride. A suitable crystal was selected and the data were collected on an Agilent Technologies SuperNova Dual Source diffractometer using a µ-focus Cu Kα radiation source (λ = Å) with collimating mirror monochromators. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S19. View of complex of 1 LiCl. Displacement ellipsoids are scaled to the50% probability level. S16
17 Table S4 Crystal data and structure refinement for 1 LiCl Empirical formula C54H69ClLiN9O7 Formula weight Temperature/K Crystal system triclinic Space group P-1 a/å (2) b/å (3) c/å (3) α/ (14) β/ (15) γ/ (17) Volume/Å (9) Z 2 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation CuKα (λ = ) 2Θ range for data collection/ to Index ranges -13 h 13, -16 k 16, -22 l 22 Reflections collected Independent reflections [Rint = , Rsigma = ] Data/restraints/parameters 10647/435/673 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-0.37 CCDC number S17
18 X-ray experimental for the complex of 1 LiBr Single crystals of C56 H65 Br Li N11 O4 [1 LiBr] were obtained as colorless blocks via the slow evaporation of a CHCl3/CH3CN/CH3OH solution of receptor 1 in the presence of excess lithium bromide. A suitable crystal was selected and the data were collected on a Rigaku AFC12 diffractometer with a Saturn 724+ CCD using a graphite. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S20. View of complex of 1 LiBr. Displacement ellipsoids are scaled to the50% probability level. S18
19 Table S5 Crystal data and structure refinement for 1 LiBr Empirical formula C56H65BrLiN11O4 Formula weight Temperature/K Crystal system triclinic Space group P-1 a/å (8) b/å (8) c/å (8) α/ (2) β/ (2) γ/ (2) Volume/Å (3) Z 2 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation MoKα (λ = ) 2Θ range for data collection/ to Index ranges -16 h 16, -16 k 16, -17 l 17 Reflections collected Independent reflections 9281 [Rint = , Rsigma = ] Data/restraints/parameters 9281/42/684 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-0.49 CCNC number S19
20 X-ray experimental for the complex of 1 LiI Single crystals of C56H65ILiN11O4 [1 LiI] were obtained as colorless blocks via the slow evaporation of a CHCl3/CH3CN/CH3OH solution of receptor 1 in the presence of excess lithium Iodide. A suitable crystal was selected and the data were collected on an Agilent Technologies SuperNova Dual Source diffractometer using a µ-focus Cu Kα radiation source (λ = Å) with collimating mirror monochromators. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S21. View of complex of 1 LiI. Displacement ellipsoids are scaled to the50% probability level. S20
21 Table S6 Crystal data and structure refinement for complex of 1 LiI Empirical formula C56H65ILiN11O4 Formula weight Temperature/K Crystal system triclinic Space group P-1 a/å (14) b/å (14) c/å (14) α/ (3) β/ (3) γ/ (3) Volume/Å (5) Z 2 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation MoKα (λ = ) 2Θ range for data collection/ to Index ranges -16 h 16, -16 k 16, -17 l 17 Reflections collected Independent reflections 9391 [Rint = , Rsigma = ] Data/restraints/parameters 9391/471/679 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-0.72 CCDC number S21
22 X-ray experimental for the complex of 1 LiNO2 Single crystals of C56 H65 Li N12 O6 [1 LiNO2] were obtained as colorless blocks via the slow evaporation of a CHCl3/CH3CN/CH3OH solution of receptor 1 in the presence of excess lithium nitrite. A suitable crystal was selected and the data were collected on an Agilent Technologies SuperNova Dual Source diffractometer using a µ-focus Cu Kα radiation source (λ = Å) with collimating mirror monochromators. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S22. View of complex of 1 LiNO 2. Displacement ellipsoids are scaled to the50% probability level. S22
23 Table S7 Crystal data and structure refinement for HQ-2N-calixpyr-LiNO2 Empirical formula C56H65LiN12O6 Formula weight Temperature/K (10) Crystal system triclinic Space group P-1 a/å (3) b/å (3) c/å (3) α/ (19) β/ (19) γ/ (2) Volume/Å (11) Z 2 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation CuKα (λ = ) 2Θ range for data collection/ to Index ranges -17 h 17, -17 k 17, -18 l 18 Reflections collected Independent reflections [Rint = , Rsigma = ] Data/restraints/parameters 10482/453/690 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-0.65 CCDC number S23
24 X-ray experimental for the complex of 1 LiNO3 Single crystals of C51 H60 Li N9 O8 [1 LiNO3] were obtained as colorless blocks via the slow evaporation of a CHCl3/CH3CN/CH3OH solution of receptor 1 in the presence of excess lithium nitrate. A suitable crystal was selected and the data were collected on a Rigaku AFC12 diffractometer with a Saturn 724+ CCD using a graphite. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S23 View of complex of 1 LiNO 3. Displacement ellipsoids are scaled to the50% probability level. S24
25 Table S8 Crystal data and structure refinement for the complex of 1 LiNO3 Empirical formula C51H60LiN9O8 Formula weight Temperature/K Crystal system monoclinic Space group P21/c a/å (9) b/å (7) c/å (16) α/ 90 β/ (2) γ/ 90 Volume/Å (5) Z 4 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation MoKα (λ = ) 2Θ range for data collection/ 6.11 to Index ranges -17 h 17, -14 k 14, -32 l 32 Reflections collected Independent reflections 8592 [Rint = , Rsigma = ] Data/restraints/parameters 8592/417/635 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-0.80 CCDC number S25
26 X-ray experimental for 1 2H2O Single crystals of C50 H60 N8 O6 [1 2H2O] were obtained as colorless blocks via the slow evaporation of a CHCl3/CH3OH solution of receptor 1. A suitable crystal was selected and the data were collected on a Rigaku AFC12 diffractometer with a Saturn 724+ CCD using a graphite. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S24. View of complex of 1 2H 2O. Displacement ellipsoids are scaled to the50% probability level. S26
27 Table S9 Crystal data and structure refinement for 1 2H2O Empirical formula C64HClLiN4O4 Formula weight Temperature/K Crystal system triclinic Space group P-1 a/å 9.700(2) b/å (3) c/å (5) α/ (15) β/ (7) γ/ (7) Volume/Å (9) Z 2 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation MoKα (λ = ) 2Θ range for data collection/ to Index ranges -12 h 12, -13 k 15, -25 l 26 Reflections collected Independent reflections [Rint = , Rsigma = ] Data/restraints/parameters 10304/384/592 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-1.06 CCDC number S27
28 X-ray experimental for 1 2CH3OH Single crystals of C105 H136 N16 O15 [1 2CH3OH] were obtained as colorless blocks via the slow evaporation of an Ethyl acetate/ch3oh solution of receptor 1. A suitable crystal was selected and the data were collected on a Rigaku SCX-Mini diffractometer with a Mercury CCD using a graphite. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S25. View of complex of 1 2CH 3OH. Displacement ellipsoids are scaled to the50% probability level. S28
29 Table S10 Crystal data and structure refinement for 1 2CH3OH Empirical formula C48H28N6O4Cl0.17 Formula weight Temperature/K Crystal system triclinic Space group P-1 a/å (6) b/å (11) c/å (13) α/ (2) β/ (2) γ/ (2) Volume/Å (5) Z 6 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation MoKα (λ = ) 2Θ range for data collection/ 6.03 to Index ranges -14 h 14, -26 k 26, -30 l 30 Reflections collected Independent reflections [Rint = , Rsigma = ] Data/restraints/parameters 22854/810/1258 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-1.22 CCDC number S29
30 X-ray experimental for 1 CH3CN Single crystals of C102 H112 N18 O7 [1 CH3CN] were obtained as colorless blocks via the slow evaporation of an acetonitrile solution of receptor 1. A suitable crystal was selected and the data were collected on a Rigaku SCX-Mini diffractometer with a Mercury CCD using a graphite. The crystal was kept at K during data collection. Using Olex2 5, the structure was solved with the ShelXT 6 structure solution program using Direct Methods and refined with the ShelXL 7 refinement package using Least Squares minimisation. Tables of positional and thermal parameters, bond lengths and angles, torsion angles and figures are in the CIF. CCDC deposition number: Figure S26. View of complex of 1 CH 3CN. Displacement ellipsoids are scaled to the50% probability level. S30
31 Table S11 Crystal data and structure refinement for 1 CH3CN Empirical formula C102 H112 N18 O7 Formula weight Temperature/K Crystal system triclinic Space group P-1 a/å (19) b/å (3) c/å (3) α/ (3) β/ (4) γ/ (4) Volume/Å (12) Z 6 ρcalcg/cm μ/mm F(000) Crystal size/mm Radiation MoKα (λ = ) 2Θ range for data collection/ 5.97 to Index ranges -18 h 17, -23 k 24, -26 l 26 Reflections collected Independent reflections [Rint = , Rsigma = ] Data/restraints/parameters 21702/0/1163 Goodness-of-fit on F Final R indexes [I>=2σ (I)] R1 = , wr2 = Final R indexes [all data] R1 = , wr2 = Largest diff. peak/hole / e Å /-0.52 CCDC number S31
32 9. REFERENCES (1). Chan, Julian M.W.; Swager, Timothy M. Tetrahedron Lett. 2008, 49, (2). (a) Park, I. W.; Yoo, J.; Kim, B.; Adhikari, S.; Kim, S. K.; Yeon, Y.; Haynes, C. J. E.; Sutton, J. L.; Tong, C. C.; Lynch, V. M.; Sessler, J. L.; Gale, P. A.; Lee, C. H. Chem. -Eur. J. 2012, 18, 2514; (b) Park, I. W.; Yoo, J.; Adhikari, S.; Park, J. S.; Sessler, J. L.; Lee, C. H. Chem. Eur. J. 2012, 18, (3). Kim, S. K.; Sessler, J. L. Acc. Chem. Res. 2014, 47, (4). Gaussian 09, Revision E.01, Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M. A.; Cheeseman, J. R.; Scalmani, G.; Barone, V.; Mennucci, B.; Petersson, G. A.; Nakatsuji, H.; Caricato, M.; Li, X.; Hratchian, H. P.; Izmaylov, A. F.; Bloino, J.; Zheng, G.; Sonnenberg, J. L.; Hada, M.; Ehara, M.; Toyota, K.; Fukuda, R.; Hasegawa, J.; Ishida, M.; Nakajima, T.; Honda, Y.; Kitao, O.; Nakai, H.; Vreven, T.; Montgomery, Jr., J. A.; Peralta, J. E.; Ogliaro, F.; Bearpark, M.; Heyd, J. J.; Brothers, E.; Kudin, K. N.; Staroverov, V. N.; Kobayashi, R.; Normand, J.; Raghavachari, K.; Rendell, A.; Burant, J. C.; Iyengar, S. S.; Tomasi, J.; Cossi, M.; Rega, N.; Millam, J. M.; Klene, M.; Knox, J. E.; Cross, J. B.; Bakken, V.; Adamo, C.; Jaramillo, J.; Gomperts, R.; Stratmann, R. E.; Yazyev, O.; Austin, A. J.; Cammi, R.; Pomelli, C.; Ochterski, J. W.; Martin, R. L.; Morokuma, K.; Zakrzewski, V. G.; Voth, G. A.; Salvador, P.; Dannenberg, J. J.; Dapprich, S.; Daniels, A. D.; Farkas, Ö.; Foresman, J. B.; Ortiz, J. V.; Cioslowski, J.; and Fox, D. J., Gaussian, Inc., Wallingford CT, (5). Dolomanov, O.V., Bourhis, L.J., Gildea, R.J, Howard, J.A.K. & Puschmann, H. (2009), J. Appl. Cryst. 42, (6). Sheldrick, G.M. Acta Cryst. 2015, A71, 3. (7). Sheldrick, G.M. Acta Cryst. 2015, C71, 3. S32
33 10. Energies and geometrical coordinates of the optimized models in the gas phase Receptor 1 E(RB3LYP): a.u. Number of negative frequencies: 0 Cartesian coordinates: Symbol X Y Z C C H C H C C C C H C H C C C C H C H C C C C H C H C C C H H H C H H S33
34 H C H H H C H H H C H H H C H H H C H H C H H C C C H C H C H C C C H C H C H C C S34
35 C C H C H C H C C C H H C H H C H H H N N N N N N N N H O O O H H H H H Complex of 1 LiCl E(RB3LYP): a.u. Number of negative frequencies: 0 Cartesian coordinates: S35
36 Symbol X Y Z C C H C H C C C C H C H C C C C H C H C C C C H C H C C C H H H C H H H C H H H S36
37 C H H H C H H H C H H H C H H C H H C C C H C H C H C C C H C H C H C C C C H C H S37
38 C H C C C H H C H H C H H H Li N N N N N N N N H O O O H H H H H Cl Complex of 1 NaCl E(RB3LYP): a.u. Number of negative frequencies: 0 Cartesian coordinates: Symbol X Y Z C C S38
39 H C H C C C C H C H C C C C H C H C C C C H C H C C C H H H C H H H C H H H C H H S39
40 H C H H H C H H H C H H C H H C C C H C H C H C C C H C H C H C C C C H C H C H C S40
41 C C H H C H H C H H H N N N N N N N N H O O O H H H H H Cl Na Complex of 1 KCl E(RB3LYP): a.u. Number of negative frequencies: 0 Cartesian coordinates: Symbol X Y Z C C H C H S41
42 C C C C H C H C C C C H C H C C C C H C H C C C H H H C H H H C H H H C H H H C H S42
43 H H C H H H C H H C H H C C C H C H C H C C C H C H C H C C C C H C H C H C C C H S43
44 H C H H C H H H N N N N N N N N H O O O H H H H H Cl K Complex of 1 LiCl H 2O E(RB3LYP): a.u. Number of negative frequencies: 0 Cartesian coordinates: Symbol X Y Z C C H C H C C C S44
45 C H C H C C C C H C H C C C C H C H C C C H H H C H H H C H H H C H H H C H H H C S45
46 H H H C H H C H H C C C H C H C H C C C H C H C H C C C C H C H C H C C C H H C H S46
47 H C H H H Li N N N N N N N N H O O O O H H H H H H H Cl Complex of 1 NaCl H 2O E(RB3LYP): a.u. Number of negative frequencies: 0 Cartesian coordinates: Symbol X Y Z C C H C H C C C S47
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