22.03.2013 Views

et al.

et al.

et al.

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

ferent structures rather than the expansion of ring<br />

sizes in the channels. In this study, we used the<br />

zinc-g<strong>al</strong>lium bim<strong>et</strong><strong>al</strong>lic system and found that<br />

increasing the template from 4C-containing (4C´)<br />

butylamine to 6C´ hexylamine was sufficient to<br />

enlarge the channel sizes from 24R to 28R, creating<br />

28R-NTHU-13 with a channel diam<strong>et</strong>er exceeding<br />

1 nm (Table 1). In subsequent reactions<br />

[table S2 (26)], the use of longer amine (8C´<br />

octylamine, 10C´ decylamine, or 12C´ dodecylamine)<br />

created the larger ring products 40R- and<br />

48R-NTHU-13, respectively. The use of 14C´<br />

t<strong>et</strong>radecylamine, 16C´ hexadecylamine, and 18C´<br />

octadecylamine led to the synthesis of 56R-<br />

NTHU-13, 64R-NTHU-13, and 72R-NTHU-13<br />

in which pore sizes were as large as 3.5 nm<br />

(Table 1).<br />

We used single-cryst<strong>al</strong> x-ray diffraction to<br />

characterize <strong>al</strong>l six structures in the NTHU-13<br />

family (figs. S1 to S10 and table S3). Four channels<br />

were d<strong>et</strong>ermined in the unit cells for 40R-,<br />

48R-, 56R-, 64R-, and 72R-NTHU-13 (Fig. 1A),<br />

and eight channels were found in the orthorhombic<br />

cell for 28R-NTHU-13 (fig. S3). Except for<br />

the latter, the channel w<strong>al</strong>ls were constructed exclusively<br />

from the following three building blocks:<br />

anionic chains of ∞[GaF(HPO 3) 2] 2– (block A),<br />

neutr<strong>al</strong> chains of ∞[Zn(HPO3)] (block B), and an<br />

anionic trimeric cluster of [Zn(HPO 3) 2(H 2O) 4] 2–<br />

(block C) (Fig. 2). Block A was located at the<br />

four corners of the square-shaped channels (Fig.<br />

2A); both A and C were linked only to B and<br />

were never adjacent. A gener<strong>al</strong>ized formula of<br />

[A(BC)nBA] describes the stoichiom<strong>et</strong>ry and connectivity<br />

of the four faces or edges of the inorganic<br />

w<strong>al</strong>ls: n = 1 for each face or edge of the<br />

40R channel, n = 2 for the 56R channel, and n =3<br />

for the 72R channel. When n = 0, the corresponding<br />

channel face is ABA and is observed to<br />

form 24R channels. Hence, the 40R, 56R, and<br />

72R square-windowed channels can be viewed<br />

as the systematic expansion of the 24R channel<br />

by inserting one or more BC pairs as the proliferation<br />

unit (Fig. 2B). The rectangular-windowed<br />

48R and 64R channels contain two mixed n v<strong>al</strong>ues<br />

(n and n + 1) to describe the shorter and<br />

longer window edges (Table 1 and table S4). An<br />

increase of one BC pair would add four polyhedra<br />

to each channel edge, leading to an expansion<br />

by 16 rings for square-windowed channels (24R<br />

to 40R; 40R to 56R; 56R to 72R) and 8 rings for<br />

rectangular-windowed channels (40R to 48R; 48R<br />

to 56R; 56R to 64R; 64R to 72R).<br />

For each 8-ring expansion, there was an approximate<br />

0.8-nm increase in the channel diam<strong>et</strong>er<br />

and an ~18 Å increase in the unit cell length<br />

(Table 1) in addition to a periodic change in the<br />

w<strong>al</strong>l structure symm<strong>et</strong>ry. As illustrated in Fig. 3,<br />

the w<strong>al</strong>l structure shows 2/m symm<strong>et</strong>ry <strong>al</strong>ong a<br />

(or b)whenn = 1 (or for odd numbers); however,<br />

2/c symm<strong>et</strong>ry is observed when n = 2 (or for even<br />

numbers). These results explain why both 40Rand<br />

72R-NTHU-13 are in the I41/amd space group,<br />

56R-NTHU-13 belongs in space group I4 1/acd,<br />

and the orthorhombic 48R- and 64R-NTHU-13<br />

possess both the m and c glide planes in their<br />

space group symm<strong>et</strong>ry. Notably, each BC pair<br />

incorporates addition<strong>al</strong> zinc ions and phosphite<br />

groups into the framework at a fixed 5:6 ratio,<br />

which causes the Ga concentration to decrease as<br />

the channels are expanded. The h<strong>et</strong>erom<strong>et</strong><strong>al</strong> centers<br />

of Ga 3+ provide the NTHU-13 family with a<br />

key structur<strong>al</strong> component: block A. When n = ∞,<br />

the NTHU-13 system would reach a maximum<br />

M/P v<strong>al</strong>ue of 5/6 (where M is the tot<strong>al</strong> number of<br />

Zn and Ga centers, and P is the number of phosphite<br />

groups) and would form lamellar structures.<br />

The 56R and 72R channels (with free diam<strong>et</strong>ers<br />

of 2.52 nm and 3.5 nm, respectively) are<br />

in the mesopore regime, which is a mesoporous<br />

framework with t<strong>et</strong>ragon<strong>al</strong> symm<strong>et</strong>ry showing<br />

regularly spaced inorganic channels with ordered<br />

w<strong>al</strong>l structures at the atomic level (27). Among<br />

<strong>al</strong>l reported cryst<strong>al</strong>line inorganic frameworks to<br />

date, 72R-NTHU-13 possesses the lowest framework<br />

density (5.28) and the highest nonframework<br />

volume (75.7%) (table S1). The channel<br />

space was parti<strong>al</strong>ly occupied by organized assemblies<br />

of monoprotonated amine molecules<br />

(~50%) with a density near that of the pure<br />

molecular liquid or solid state (Table 1). The templates<br />

were distributed quite near the inorganic<br />

w<strong>al</strong>l with their ammonium heads pointing primarily<br />

toward the negatively charged blocks A<br />

and C (and are <strong>al</strong>so likely to contain hydrogen<br />

bonds, because the closest N … O distances were<br />

observed to f<strong>al</strong>l in the range of 2.83 to 2.90 Å).<br />

Their long carbon chain skel<strong>et</strong>ons were disordered<br />

and pointed toward the hydrophobic region of the<br />

channel centers (fig. S9). Within each of the 56R,<br />

64R, or 72R channels per unit cell, there exist 16,<br />

18, or 20 monoprotonated template-amine molecules.<br />

Element<strong>al</strong> an<strong>al</strong>ysis data (table S5) and<br />

solid-state nuclear magn<strong>et</strong>ic resonance studies<br />

using 1 H, 13 C, and 19 F confirmed the content of<br />

the organic templates and the presence of fluoride<br />

(figs. S11 to S13).<br />

Thermogravim<strong>et</strong>ric an<strong>al</strong>ysis (fig. S14) combined<br />

with variable-temperature powder x-ray<br />

diffraction measurements (fig. S15) were used to<br />

d<strong>et</strong>ermine the therm<strong>al</strong> stability of 40R-, 48R-,<br />

and 56R-NTHU-13, which were therm<strong>al</strong>ly stable<br />

up to 175°C. When transparent colorless cryst<strong>al</strong>s<br />

of 40R-NTHU-13 were treated with 0.05 M<br />

parafuchsin hydrochloride (in <strong>et</strong>hanol), the<br />

cryst<strong>al</strong>s changed to a pink color (fig. S16), which<br />

indicates that the dye molecules were adsorbed.<br />

Cs + ion exchange was performed by treating powder<br />

samples of 40R- and 48R-NTHU-13 with a<br />

0.01 M CsCl <strong>et</strong>hanol solution, and positive results<br />

were confirmed by x-ray fluorescence data<br />

in combination with powder x-ray diffraction<br />

measurements (table S6 and fig. S17). The empty<br />

space inside the channels was d<strong>et</strong>ected even in<br />

the presence of the residu<strong>al</strong> templates, as indicated<br />

by preliminary results from gas adsorption<br />

measurements performed on 56R-NTHU-13 samples<br />

(fig. S18).<br />

Relative to the <strong>al</strong>uminosilicates, the cryst<strong>al</strong>s<br />

of NTHU-13 are less robust in nature, and so far<br />

have not y<strong>et</strong> shown impressive convention<strong>al</strong> porerelated<br />

properties such as gas sorption (the maximum<br />

CO2 uptake of 56R-NTHU-13 at 1 atm is<br />

0.32 mmol/g; see figs. S18 and S19). However,<br />

very large inorganic channels may display unexpected<br />

properties such as pore-related photoluminescence,<br />

as we previously reported (5–7). When the<br />

40R channel framework was successfully doped<br />

with Mn 2+ ions, an unusu<strong>al</strong> broad band of nearly<br />

white light emission under ultraviol<strong>et</strong> excitation was<br />

displayed by the resultant Mn@40R-NTHU-13<br />

(fig. S20). Thus, the host lattice of 40R-NTHU-13<br />

reve<strong>al</strong>ed the ability to create a white-light phosphor<br />

from single-activator doping.<br />

References and Notes<br />

1. A. Corma, Chem. Rev. 97, 2373 (1997).<br />

2. M. E. Davis, Nature 417, 813 (2002).<br />

3. H. Furukawa <strong>et</strong> <strong>al</strong>., Science 329, 424 (2010).<br />

4. Y. S. Bae, R. Q. Snurr, Angew. Chem. Int. Ed. 50, 11586<br />

(2011).<br />

5. Y. C. Liao, C. H. Lin, S. L. Wang, J. Am. Chem. Soc. 127,<br />

9986 (2005).<br />

6. Y. C. Yang, S. L. Wang, J. Am. Chem. Soc. 130, 1146<br />

(2008).<br />

7. P. C. Jhang, Y. C. Yang, Y. C. Lai, W. R. Liu, S. L. Wang,<br />

Angew. Chem. Int. Ed. 48, 742 (2009).<br />

8. S. T. Wilson, B. M. Lok, C. A. Messina, T. R. Cannan,<br />

E. M. Flanigen, J. Am. Chem. Soc. 104, 1146 (1982).<br />

9. P. B. Moore, J. Shen, Nature 306, 356 (1983).<br />

10. M. E. Davis, C. S<strong>al</strong>darriaga, C. Montes, J. Garces,<br />

C. Crowdert, Nature 331, 698 (1988).<br />

11. M. Estermann, L. B. McCusker, C. Baerlocher,<br />

A. Merrouche, H. Kessler, Nature 352, 320 (1991).<br />

12. C. C. Freyhardt, M. Tsapatsis, R. F. Lobo, K. J. B<strong>al</strong>kus Jr.,<br />

M. E. Davis, Nature 381, 295 (1996).<br />

13. N. Guillou <strong>et</strong> <strong>al</strong>., Angew. Chem. Int. Ed. 40, 2831 (2001).<br />

14. G.-Y. Yang, S. C. Sevov, J. Am. Chem. Soc. 121, 8389<br />

(1999).<br />

15. C. H. Lin, S. L. Wang, K. H. Lii, J. Am. Chem. Soc. 123,<br />

4649 (2001).<br />

16. X. Zou, T. Conradsson, M. Klingstedt, M. S. Dadachov,<br />

M. O’Keeffe, Nature 437, 716 (2005).<br />

17. Y. L. Lai, K. H. Lii, S. L. Wang, J. Am. Chem. Soc. 129,<br />

5350 (2007).<br />

18. J. Sun <strong>et</strong> <strong>al</strong>., Nature 458, 1154 (2009).<br />

19. N. L. Rosi <strong>et</strong> <strong>al</strong>., Science 300, 1127 (2003).<br />

20. H. Deng <strong>et</strong> <strong>al</strong>., Science 336, 1018 (2012).<br />

21. M. V. Peskov, X. Zou, J. Phys. Chem. C 115, 7729 (2011).<br />

22. L. Tang <strong>et</strong> <strong>al</strong>., Nat. Mater. 7, 381 (2008).<br />

23. C. T. Kresge, M. E. Leonowicz, W. J. Roth, J. C. Vartuli,<br />

J. S. Beck, Nature 359, 710 (1992).<br />

24. Q. Huo <strong>et</strong> <strong>al</strong>., Nature 368, 317 (1994).<br />

25. Microporous pores and channels have pore diam<strong>et</strong>ers (d) <<br />

2.0 nm, whereas mesoporous ones have 2.0 ≤ d ≤ 50 nm.<br />

26. See supplementary materi<strong>al</strong>s on Science Online.<br />

27. The cryst<strong>al</strong>line inorganic framework will collapse if the<br />

organic template is compl<strong>et</strong>ely removed.<br />

28. A. L. Spek, Acta Cryst<strong>al</strong>logr. A 46, C34 (1990).<br />

Acknowledgments: Supported by Nation<strong>al</strong> Science<br />

Council of Taiwan grants NSC100-2113-M-007-016-MY3,<br />

NSC101-2113-M-033-007-MY3, and NSC101-2113-M-008-006-MY3.<br />

X.B. was supported by NSF grant DMR-0846958. Cryst<strong>al</strong>lographic<br />

data for the reported cryst<strong>al</strong> structures have been deposited<br />

at the Cambridge Cryst<strong>al</strong>lographic Data Centre with<br />

codes 892384–892387 and 915187–915191.<br />

Supplementary Materi<strong>al</strong>s<br />

www.sciencemag.org/cgi/content/full/339/6121/811/DC1<br />

Materi<strong>al</strong>s and M<strong>et</strong>hods<br />

Figs. S1 to S20<br />

Tables S1 to S6<br />

References (29–36)<br />

29 October 2012; accepted 14 December 2012<br />

10.1126/science.1232097<br />

REPORTS<br />

www.sciencemag.org SCIENCE VOL 339 15 FEBRUARY 2013 813<br />

Downloaded from<br />

www.sciencemag.org on February 14, 2013

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!