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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 />
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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 />
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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 />
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