# Nanoconfinement-Induced Electrochemical Ion-Solvent Cointercalation in Pillared Titanate Host Materials

Mennatalla Elmanzalawy, Haohong Song, Maciej Tobis, Robert Leiter, Jaehoon Choi, Hyein Moon, Wan-Yu Tsai, De-en Jiang, Simon Fleischmann

► To cite this version:

Mennatalla Elmanzalawy, Haohong Song, Maciej Tobis, Robert Leiter, Jaehoon Choi, et al. Nanoconfinement-Induced Electrochemical Ion-Solvent Cointercalation in Pillared Titanate Host Materials. Angewandte Chemie International Edition, 2025, 10.1002/anie.202423593. [https://doi.org/10.1002/anie.202423593](https://doi.org/10.1002/anie.202423593). [arXiv:2409.05173](https://arxiv.org/abs/2409.05173)

HAL Id: hal-04995173

https://hal.science/hal-04995173v1

Submitted on 18 Mar 2025

**HAL** is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L'archive ouverte pluridisciplinaire **HAL**, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d'enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

<figure><img src="image_1.png" /></figure>

Distributed under a Creative Commons Attribution 4.0 International License
# Nanoconfinement-Induced Electrochemical Ion-Solvent Cointercalation in Pillared Titanate Host Materials

Mennatalla Elmanzalawy, Haohong Song, Maciej Tobis, Robert Leiter, Jaehoon Choi, Hyein Moon, Wan-Yu Tsai, De-en Jiang, and Simon Fleischmann*

**Abstract:** Electrochemical ion-solvent cointercalation reactions are an avenue to reach improved kinetics compared to the corresponding intercalation of desolvated ions. Here, we demonstrate the impact of different structural pillar molecules on the electrochemical $Li^+$ intercalation mechanism in expanded hydrogen titanate (HTO) electrode materials. We show that interlayer-expansion of HTO with organic pillars can enable cointercalation reactions. Their electrochemical reversibility is drastically improved when non-cross-linking pillars are employed that expand and separate the host material's individual layers, underlining the impact of the electrochemo-mechanics of the nanoconfined interlayer space. This pillared HTO structure results in an increased $Li^+$ storage capacity and reversibility compared to pristine HTO. We derive structural models of the pillared HTO host materials based on combined experiments and theoretical calculations, and employ electrochemical operando experiments to unambiguously demonstrate the nanoconfinement-induced cointercalation mechanism in pillared HTO electrode materials. The work demonstrates the potential of nanoconfined pillar molecules to modify host materials and enable highly reversible cointercalation reactions with improved capacity and kinetics.

Received: 29.December 2024

## 1. Introduction

Electrochemical energy storage devices, including lithium-ion and sodium-ion batteries, are in increasing global

demand. Their functioning mechanism is the electrochemical intercalation of ions from the electrolyte into the solid-state host structure of the electrode materials. Layered transition metal oxides (TMOs) are widely used as cathode materials and serve as alternatives to carbon-based anodes in lithium- and sodium-ion batteries. Among them, titanate-based materials have attracted interest due to their relative abundance, low toxicity and structural/chemical tunability. They can often serve as host structures for both lithium- and sodium-ions making them highly versatile.[1-3]

Hydrogen titanates are a family of metastable materials derived from layered alkali titanates.[4,5] They are typically synthesized in acidic solution by etching and topotactic exchange of the alkali ion in the interlayer space by protons and/or water.[5-7] This provides them with a high degree of structural/chemical tunability of their nanoconfined interlayer composition, comparable to two-dimensional $Ti_3C_2T_xMXenes$ derived via a similar selective etching approach.[8,9] These materials' nanoconfinement environment, in turn, can have an effect on their electrochemical ion intercalation properties.[10-13]

In the layered hydrogen titanate $H_2Ti_3O_7$, it was found that confined interlayer protons are the determining structural feature to enable electrochemical $H^+$ intercalation.[14] This is because they separate the titanate layers, allowing to effectively compensate electrochemically induced strain by contraction/expansion without altering intralayer structure.[14] Interlayer-expansion of layered titanate hollow spheres by confined $Mg^{2+}$ ions was demonstrated as a design strategy for electrochemical $Na^+$ intercalation hosts.[15] An investigation into different types of confined alkali ions ($Li^+$, $Na^+$, $K^+$, $Cs^+$) within lepidocrocite-type layered titanates revealed that the interlayer spacing is expanded with increasing ion size (0.68 to 0.85 nm).[16] However, sodium-

[*] M. Elmanzalawy, M. Tobis, R. Leiter, J. Choi, H. Moon, S. Fleischmann
Helmholtz Institute Ulm (HIU), 89081 Ulm, Germany
E-mail: simon.fleischmann@kit.edu

M. Elmanzalawy, M. Tobis, R. Leiter, J. Choi, H. Moon, S. Fleischmann
Karlsruhe Institute of Technology (KIT), 76021 Karlsruhe, Germany

H. Song
Interdisciplinary Materials Science, Vanderbilt University, Nashville, Tennessee, 37235, United States

W.-Y. Tsai
Univ. Lille, CNRS, Univ. Polytechnique Hauts-de-France, UMR 8520 - IEMN, F-59000 Lille, France

W.-Y. Tsai
Réseau sur le Stockage Electrochimique de l'Energie (RS2E), CNRS FR 3459, 33 rue Saint Leu, Amiens, Cedex 80039, France

D.-e. Jiang
Department of Chemical and Biomolecular Engineering, Vanderbilt University, Nashville, Tennessee, 37235, United States

© 2025 The Author(s). Angewandte Chemie International Edition published by Wiley-VCH GmbH. This is an open access article under the terms of the Creative Commons Attribution License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
modified titanate showed the highest capacity for electro-
chemical Na⁺ intercalation hosts (153 mAh g⁻¹), even
though this material has a smaller interlayer spacing than
the cesium-modified titanate (95 mAh g⁻¹), demonstrating
the importance of nanoconfinement chemistry in addition to
just geometrical considerations.[16] In the layered hydrogen
titanate H₂Ti₂O₅ system, it was found that K⁺ intercalation
can be accomplished most efficiently, especially at low
temperatures (−40 °C), for the material with confined
interlayer water (H₂Ti₂O₅·H₂O, “HTO”), compared to its
dehydrated form with additional interlayer defects (“QTO”)
that also exhibits smaller interlayer spacing (0.78 nm for
QTO vs. 0.84 nm for HTO).[17] The authors attribute this to
ion-solvent cointercalation from the organic electrolyte into
HTO, which is enabled by strong K⁺/1,2-dimethoxyethane
binding energy (electrolyte effect) and a charge shielding
effect of confined interlayer H₂O (electrode effect).[17] The
emergence of such cointercalation phenomena is gaining
more and more interest, as it offers the opportunity to
substantially modifying electrode reactions regarding redox
potential, capacity and kinetics and even enable reactions
not feasible for desolvated ions.[18–21] However, the phenom-
enon is almost exclusively studied as an electrolyte effect,
while the influence of the electrode on cointercalation is
widely neglected.[22]

This motivates us to explore the structural motifs that
enable such favorable electrochemical cointercalation effects
in titanates. Besides interlayer modification of layered
titanates with simple cations or crystal water, the introduc-
tion of organic pillar molecules like linear alkyl (di)amines
offers an even wider materials design space,[23–27] with the
potential to induce effective cointercalation phenomena.[22]
However, no clear materials design rules for host materials
on how to control cointercalation have emerged so far.
Specifically, there is an urgent need to identify how electro-
chemically induced strain is compensated in strongly
expanded/pillared titanates and whether layer-separating or
cross-linking pillaring approaches favor electrochemical
kinetics.

In this work, we investigate the layered titanate
H₂Ti₄O₉·H₂O and increase its interlayer spacing from 0.88 to
1.58 nm by insertion of organic molecular pillars. This first
step enables the study of nanoconfinement geometry's
influence on electrochemical ion intercalation. Furthermore,
using either propylamine (PA) or 1,6-hexanediamine
(HDA) pillars, an identical expanded interlayer spacing is
obtained. But while HDA pillars with two ammonium
groups cross-link the titanate layers, PA pillars are non-
cross-linking, likely impacting how electrochemically-in-
duced strain is compensated within the host lattice. We
utilize a combination of experimental and theoretical
methods to derive precise structural models of the pillared
titanates. Electrochemical Li⁺ intercalation capacity from
organic electrolyte can be increased from ca. 2.1 to 2.95 Li⁺
per tetratitanate when pillaring with non-cross-linking PA
molecules. Using a combination of operando X-ray diffrac-
tion (XRD), electrochemical dilatometry (ECD) and elec-
trochemical quartz crystal microbalance (EQCM), we un-
ambiguously identify a nanoconfinement-induced change in

intercalation mechanism from solid-solution intercalation to
ion-solvent cointercalation.

## 2. Results and Discussion

2.1. Physicochemical Characterization

Layered potassium tetratitanate is synthesized via a solid-
state synthesis of TiO₂ and K₂CO₃ at 800 °C, yielding
monoclinic K₂Ti₄O₉ (KTO) with a rod-like morphology
(Figure S1). The confined interlayer potassium is subse-
quently exchanged by protons and water via treatment in
HCl according to earlier work of Izawa et al.[6] The resulting
hydrogen tetratitanate H₂Ti₄O₉·H₂O (HTO) retains the rod-
like morphology of KTO as indicated by scanning electron
microscopy (SEM, Figure 1A). The rods measure up to
several microns in lengths and several hundreds of nano-
meters in diameter, in agreement with previous reports.[28]
The chemical composition of the nanoconfined interlayer
environment of HTO can be further modified with organic
amine-based molecular pillars replacing interlayer water[23]
without leading to any visible modification of the macro-
scopic rod-like morphology as shown by SEM micrographs
(Figure 1B–C). Propylamine (PA) and 1,6-hexanediamine
(HDA) are selected as molecular pillars with one or two
anchoring amine groups, respectively. The reason is the
assumption that monofunctional PA bonds to one layer of
the titanate host resulting in a separated HTO structure,
while bifunctional HDA interacts with two adjacent titanate
layers leading to a cross-linked HTO structure. Hence the
pillar choice allows to compare the influence of interconnec-
tivity of the pillared structure on the volumetric expansion
behavior when used as electrochemical ion intercalation
hosts.

To examine the pillar-induced changes in crystal struc-
ture, powder X-ray diffraction (XRD) patterns of the
pristine HTO and the molecularly pillared HTO-PA and
HTO-HDA are shown in Figure 1D. The XRD pattern of
as-synthesized HTO is in close agreement with that reported
in literature (PDF 00-036-0655), which indicates the success-
ful synthesis of the protonated/hydrated phase from the
precursor K₂Ti₄O₉. ICP results (Table S1) show that only
negligible amounts of potassium remain in the structure (ca.
0.2 wt.%), indicating successful ion exchange by acid treat-
ment. The introduction of molecular pillars causes a
significant shift in the (200) plane peak to lower angles,
indicative of an increase in the interlayer spacing from
0.88 nm in the pristine HTO to 1.58 nm in both HTO-PA
and HTO-HDA. The similar interlayer spacing and mor-
phology of the two molecularly pillared titanates, HTO-PA
and HTO-HDA, permits to exclusively assess the impact of
cross-linking versus layer-separating/non-cross-linking mo-
lecular pillars on the electrochemical properties.

Quantification of nanoconfined interlayer molecules
(water, or organic pillars) is conducted using thermogravi-
metric analysis (TGA, Figure 1E). Heating to 600 °C in
synthetic air atmosphere converts H₂Ti₄O₉ into 4 TiO₂ by
dehydration/dehydroxylation[29,30] (corresponding to 94.7 %
<figure><img src="image_2.png" /><figcaption>**Figure 1.** Structure and composition of HTOs: Scanning electron microscopy images of (A) H₂Ti₄O₉·H₂O (HTO), (B) HTO-HDA and (C) HTO-PA. (D) Powder XRD patterns of HTO, HTO-PA, HTO-HDA, and the PDF of H₂Ti₄O₉·H₂O as reported in the literature. (E) TGA and dTG (derivative thermogravimetry) plots for HTO, HTO-PA and HTO-HDA, showing mass loss steps and quantities. Optimized crystal structures of (F) HTO-PA and (G) HTO-HDA, obtained from DFT calculations and considering structural formulae derived from TGA (legend for atom assignment: light grey: Ti, red: O, white: H, blue: N, dark grey: C).</figcaption></figure>

of the initial mass). At the same time, there is a complete removal of nanoconfined molecular species by combustion and/or evaporation, hence any additional mass loss can be attributed to interlayer molecules.[14] For pristine HTO, an overall mass loss of 10.1 % is measured, indicating an initial composition with a structural formula H₂Ti₄O₉·0.99H₂O. The measured overall mass loss for HTO-PA is 24.7 %, indicating the initial composition H₂Ti₄O₉·1.47PA, and for HTO-HDA it is 28.8 % suggesting the structural formula H₂Ti₄O₉·0.96HDA. Hence it is reasonable to approximate

the nanoconfined interlayer chemistry of HTO, HTO-PA and HTO-HDA as 1 H₂O, 1.5 PA and 1 HDA molecules, respectively. These values are further utilized for theoretical calculation of the structure.

Taking into account the measured interlayer spacing of HTO-PA and HTO-HDA, as well as the quantification of nanoconfined pillaring molecules, the energetically favorable pillar conformation within the interlayer space is calculated using density functional theory (DFT, Figure 1F–G). For the HTO-PA system, we considered three config-
urations: fully perpendicular, fully parallel, and mixed models with respect to the HTO basal plane. The calculations show that in the fully perpendicular configuration, the d-spacing is only 1.38 nm, which is too short in comparison with the experimental value of 1.58 nm. As more PA molecules are aligned parallel to the basal plane, the d-spacing gradually increases. The PA bilayer structure allows the PA molecules to interact more effectively with the OH groups on both the upper and lower HTO layers. In the lowest energy configuration, this leads to proton transfer from HTO to PA involving the formation of propylammonium and resulting in a d-spacing of 1.58 nm (Figure 1F). For the HTO-HDA system, we considered two scenarios: HDA aligned parallel or perpendicular to the HTO basal plane. DFT structural optimization revealed that in the

perpendicular configuration, both NH₂ groups of HDA are protonated by the top and bottom HTO layers to form hexanediammonium in the lowest energy configuration (Figure 1G). In contrast, when HDA is aligned parallel to the basal plane, the energy is higher due to lack of ionic interaction and the d-spacing is shorter at 1.51 nm, in comparison with the experimental value.

Analysis of the structural properties of HTOs with different nanoconfinement chemistries at a nanoscale is conducted using transmission electron microscopy (TEM, Figure 2). All samples (HTO, HTO-PA and HTO-HDA) demonstrate rod-like morphology (Figure 2A-B, 2D-E, 2G-H), confirming prior SEM results. This allows to further analyze free-standing rods individually using selected area electron diffraction (SAED). The recorded patterns for

<figure><img src="image_3.png" /><figcaption>**Figure 2.** Transmission electron microscopy images and selected area electron diffraction pattern (area indicated by red circle) of (A–C) HTO, (D–F) HTO-PA, and (G–I) HTO-HDA.</figcaption></figure>
single crystals are then compared to the DFT-optimized
crystal structures to verify the proposed structural models.
For the pristine HTO sample, the SAED pattern (Fig-
ure 2C) aligns well with the simulated H₂Ti₄O₉ structure (see
supporting information for the coordinates). Specifically, the
(002) reflection yields a d-spacing of 0.56 nm, which closely
matches the 0.57 nm obtained from the calculated structure.
Similarly, the (110) and (220) reflections, with d-spacings of
0.37 nm and 0.19 nm, respectively, correspond precisely to
the values derived from the calculated pattern (0.37 nm and
0.19 nm).

For the HTO-PA sample, the SAED-measured (008) reflection with d-spacing measuring 0.29 nm was comparable to the simulated value of 0.287 nm, and the (220) reflection at 0.19 nm also agreed with the predicted value. Similarly, for the HTO-HDA sample, the SAED-derived (40-4) reflection with d-spacing of 0.30 nm and (1-10) with d-spacing of 0.38 nm were consistent with the corresponding simulated values of 0.30 nm and 0.38 nm, respectively. Overall, the TEM and SAED analysis confirm the validity of the proposed structural models for the pillared tetratitanates. Additionally, calculated XRD pattern of the structural models of HTO-PA and HTO-HDA are given in Figure S2. It should be noted that the experimental structural analysis is limited to the titanate host, while the conformation of organic pillars is indirectly concluded based on minimized free energy and previous literature reports of confined alkyl(di)amine pillars.[31-33]

The interaction between nanoconfined pillars within the interlayer and the HTO-based host lattice is analyzed by Raman spectroscopy. This allows to assess any organic pillaring-induced changes in bonding environment. The presence of organic pillars in HTO-PA and HTO-HDA is confirmed by signals in the C–H stretching region (2800 to 3000 cm⁻¹).[³⁴] Moreover, the spectra of HTO, HTO-PA and HTO-HDA are highly comparable in the wavenumber region below ca. 900 cm⁻¹ typically assigned to the Ti–O lattice vibrations,[³⁵] with no new major signals appearing. Shifts or broadening of certain signals can provide information about host-pillar interactions. In HTO, the band at 267 cm⁻¹ attributed to the Ti-OH bonds[³⁶,³⁷] blue shifts to 275 cm⁻¹ after pillaring with either PA or HDA. The Raman signals of HTO at 394, 452, 681 and 866 cm⁻¹ have previously been assigned to protonated tetratitanate.[²⁸,³⁸]

They are still present (394 and 452 cm⁻¹), red shift (681 to ca. 661 cm⁻¹) or broaden (866 cm⁻¹) after organic pillaring with PA and HDA. Other peaks arising from the organic pillars are present in HTO-PA and HTO-HDA and can be attributed to different components of the organic molecules (Figure S3). The overall strong similarity of the spectra is indicative of the tetratitanate intralayer structure remaining intact after pillaring. Slight shifts/broadening of protonated titanate related signals suggests an interaction between the organic pillars and the terminal protons of the titanate layers.

The nature of this interaction is further elucidated using X-ray photoelectron spectroscopy (XPS, Figure 3B–C). The Ti 2p region in pristine HTO and pillared HTO-PA and HTO-HDA all contain a mixture of Ti oxidation states Ti⁴⁺ and Ti³⁺ (Figure 3B). The Ti³⁺/Ti⁴⁺ signal intensity ratio increases from 0.196 in pristine HTO to 0.212 in HTO-PA and further to 0.355 in HTO-HDA. Pillaring of HTO with PA or HDA therefore results in the reduction of the average Ti oxidation state, with more reduction in the case of HTO-HDA. This could be explained by the overall higher number of amine groups in HTO-HDA compared to HTO-PA (ca. 2 versus 1.5 amine groups per H₂Ti₄O₉, respectively). The N 1s core-level spectra (Figure 3C) reveal the coexistence of NH₃⁺ and NH₂ species in the pillared materials, suggesting that the organic pillar exists in the structure in both its free and ionic (alkylammonium ion) forms.[³⁹] The ratio of NH₃⁺ to NH₂ was estimated to be ca. 4 to 1 in HTO-PA, and 2.5 to 1 in HTO-HDA, respectively. The higher NH₃⁺/NH₂ peak intensity ratio in HTO-PA suggests a higher tendency for the organic pillars to exist in their ionic form compared to HTO-HDA, where the alkyldiamine molecule might contain an ionized NH₃⁺ on one end and a neutral NH₂ on the other. Moreover, it is unlikely that covalent Ti–N bonds are forming due to the absence of a Ti–N peak at 397.2 eV.[⁴⁰] These findings agree with previous works that detected mixed NH₂ and NH₃⁺ species in alkylamine-pillared titanates[²⁷] and alkyldiamine-pillared vanadia.[³³]

## 2.2. Electrochemical Characterization

With HTO, HTO-PA and HTO-HDA samples exhibiting highly comparable morphology and intralayer crystal struc-

<figure><img src="image_4.png" /><figcaption>**Figure 3.** Analysis of host-pillar interaction. (A) Raman spectra, and XPS of (B) Ti 2p and (c) N 1s regions of HTO, HTP-PA, and HTO-HDA samples.</figcaption></figure>
ture, the influence of their interlayer properties on the lithium intercalation reaction can be analyzed. Specifically, the comparison of pristine versus pillared HTO allows to study the influence of interlayer spacing on the ion intercalation mechanism. For pillared HTOs, nanoconfined propylamine (PA) or hexanediamine (HDA) pillars lead to separated or cross-linked titanate layers, respectively. With both HTO-PA and HTO-HDA exhibiting the same interlayer spacing, insights into the impact of electrochemomechanics on the ion intercalation reaction can be gained.

Galvanostatic charge/discharge (GCD) profiles of the first five cycles of HTO, HTO-PA and HTO-HDA at 50 $mA g^{-1}$ in standard organic electrolyte (LP30) are shown in Figure 4A–C. All three samples exhibit a pronounced plateau for the lithium intercalation reaction. The reduction plateau is located at ca. 1.7 – 1.5 V for HTO and at ca. 1.5 – 1.3 V for HTO-PA and HTO-HDA, demonstrating a shift to a lower lithiation potential for pillared HTOs. All three samples exhibit comparable initial coulombic efficiencies (72–77%) with slight performance degradation over the first five cycles (least pronounced for HTO-PA). This indicates that organic pillars do not contribute to a decrease in initial efficiency or stability compared to pristine HTO.

Cyclic voltammograms at a sweep rate of 0.1 $mV s^{-1}$ (Figure 4D) give additional insights into the (de)lithiation process. The shift to a lower lithiation (reduction) potential for PA- and HDA-pillared materials is clearly visible. The position of the delithiation (oxidation) peak for the three materials is different, showing a variation of the overpotential of the (de)lithiation reaction. HTO-PA shows the lowest overpotential (ca. 150 mV) compared to HTO-HDA (ca. 280 mV) and HTO (ca. 220 mV), indicating the highest electrochemical reversibility for HTO-PA. Additionally, there is an identical very low intensity set of redox peaks visible around 1.75–1.8 V for all samples. These can be attributed to (de)lithiation of anatase $TiO_2$ impurity,[41] indicative of minor secondary phases across all three titanate samples potentially resulting from trace amounts of $TiO_2$ precursor from the solid-state synthesis of $K_2Ti_4O_9$. Since it is equally present in each sample, its influence on the overall comparability between the samples is negligible.

Quantitative analysis of the lithium intercalation capacity and kinetics is carried out by GCD at varying rates between 50–5,000 $mA g^{-1}$ (Figure 4E). The specific delithiation capacities at low rates (fifth cycle) of HTO, HTO-PA and HTO-HDA are 157, 186 and 150 $mAh g^{-1}$, respectively. There is a varying mass contribution of the different nano-confined interlayer molecules in the three samples, which are not participating in the reversible charge storage process, namely 1.0 $H_2O$, 1.5 PA, or 1.0 HDA. Normalizing the maximum reversible lithium storage capacities of the materials per tetratitanate can then be calculated as ca. 2.10 $Li^+$ for HTO, 2.95 $Li^+$ for HTO-PA, and 2.52 $Li^+$ for HTO-HDA. This demonstrates that the maximum reversible ion storage capacity per transition metal is increased in interlayer-expanded, organically pillared HTO materials. At increasing GCD rates, the performance of HTO-PA remains superior compared to HTO and HTO-HDA. This indicates superior charge storage kinetics when using the layer

separating/non-cross-linking PA pillars compared to cross-linking HDA pillars. However, the capacity retention of cross-linked HTO-HDA at high rates is still slightly higher compared to pristine HTO, indicating the general favorability of increased interlayer spacing for charge storage kinetics. This is also in line with previous reports of our group on alkyldiamine-pillared vanadium oxide host materials.[33]

The cycling stability of HTO-based materials is tested by GCD at an intermediate rate of 500 $mA g^{-1}$ (Figure 4F). The performance degradation is most severe for pristine HTO, with a retention of 36% of its initial capacity, while HTO-PA and HTO-HDA both retain about 55% of their initial capacity after 1,000 cycles. The strong performance degradation for HTOs in organic lithium ion-based systems has been observed before and attributed to hydrogen gas evolution at strongly reductive potentials.[13] This adverse effect on the cycling stability appears to be weakened in HTO-PA and HTO-HDA. We hypothesize that this is due to a stabilization of confined structural protons due to $NH^{3+}$ formation after introduction of amine groups. TEM images were recorded after cycling the show no visible signs of exfoliation or structural degradation (Figure S4). However, the (electrochemical) stability of confined interlayer species like protons, water, and organic pillars is still an underexplored topic and must be comprehensively analyzed to improve the cycling stability and Coulombic efficiency of pillared host materials.

Overall, the results demonstrate that the increased interlayer spacing of organically pillared HTOs results in an increased $Li^+$ storage capacity per Ti compared to pristine HTO. Moreover, the layer separating PA pillars result in superior charge storage kinetics with increased electrochemical reversibility compared to cross-linking HDA pillars.

Favorable kinetics for ion intercalation in HTO host materials has been ascribed to ion-solvent cointercalation phenomena before, when specially formulated electrolytes were used.[17] We hypothesize that a nanoconfinement-induced cointercalation mechanism is the origin of superior electrochemical kinetics of HTO-PA compared to HTO, which is known to exhibit solid-solution intercalation of desolvated $Li^+$. [13] Cointercalation reactions exhibit a reduced charge transfer resistance compared to the corresponding desolvated ion intercalation process, because of the circumvention of the desolvation step.[42–45] Hence, we can probe this behavior using electrochemical impedance spectroscopy (EIS) at various states of charge (“staircase potentio electrochemical impedance spectroscopy”) in a three-electrode cell setup. The Nyquist plots of HTO and HTO-PA at open circuit voltage (OCV, ca. 3.1 V vs. $Li^+/Li$) are shown in Figure 5A. An equivalent circuit consisting of the elements described in Figure S5 is used to model the impedance response of the intercalation process. Plotting the extracted charge transfer resistances clearly shows strongly reduced values for the charge storage process in HTO-PA compared to HTO across the entire potential range for intercalation and deintercalation (Figure 5B). The
<figure><img src="image_5.png" /><figcaption>**Figure 4.** Electrochemical performance of HTO and pillared HTO in the Li-ion system. (A–C) Galvanostatic charge and discharge plots of HTO, HTO-PA, and HTO-HDA showing the first 5 cycles at specific current rate 50 mA g⁻¹. (D) CVs of HTO, HTO-PA, and HTO-HDA showing the 2nd cycle, cycled at sweep rate 0.1 mV s⁻¹. (E) Rate handling of HTO, HTO-PA, and HTO-HDA, showing anodic capacity at various values of specific current and the corresponding coulombic efficiency of each cycle. (F) Cycling performance of HTO, HTO-PA, and HTO-HDA at specific current rate 0.5 A g⁻¹ and the corresponding coulombic efficiency. All measurements carried out in coin cells versus lithium metal with LP30 electrolyte at a constant temperature of 20 °C.</figcaption></figure>

results clearly support the assignment of the cointercalation mechanism in HTO-PA electrodes.

To further support the hypothesis of a nanoconfinement-induced cointercalation mechanism in HTO-PA, the lithiation-induced structural changes occurring in the different

host materials are analyzed during electrochemical cycling using *operando* XRD. The electrode materials are cycled by GCD at 50 mA g⁻¹ in a modified coin cell setup with Kapton-sealed windows, while X-ray diffractograms are continuously recorded in Debye-Scherrer geometry (trans-
<figure><img src="image_6.png" /><figcaption>**Figure 5.** (A) Electrochemical impedance spectroscopy (EIS) Nyquist plots for HTO and HTO-PA at OCV, measured in three-electrode cells, fitted using the equivalent circuit shown in the inset. (B) R<sub>ct</sub> values at different stages of lithiation and delithiation for HTO and HTO-PA. Error bars are based on two measurements.</figcaption></figure>

mission) with a focus on the signal representative of the interlayer spacing, i.e., the (200) set of planes. For pristine HTO, a continuous shift towards smaller interlayer spacing is observed during electrochemical lithiation (Figure 6A), indicating a contraction of titanate layers upon insertion of a positive charge in the interlayer space. In the fully lithiated state, the HTO interlayer spacing contracted from ca. 0.8 to 0.74 nm. The interlayer spacing reversibly expands to its initial value after full electrochemical delithiation, suggesting a solid-solution intercalation mechanism of Li⁺. The behavior is fully reversible and is in line with previous observations of interlayer contraction of titanates upon both proton or lithium insertion.[13,14]

For HTO-PA, the operando XRD profiles show a different behavior (Figure 6B). For interlayer-expanded HTO-PA, upon lithiation, the interlayer spacing further increases from 1.54 nm to ca. 1.68 nm. Upon delithiation, a further expansion to ca. 1.73 nm is observed. Similar observations are made for HTO-HDA (Figure S6). Furthermore, in the second lithiation cycle, the signal corresponding to the (200) plane loses intensity for HTO-PA, which indicates a loss of long-range crystalline order. The observations support the insertion of a large intercalant in HTO-PA (e.g., a partially solvated Li⁺), which apparently leads to stronger structural changes of the host lattice compared to pristine HTO. The results are fully in line with the transition from solid-solution intercalation of desolvated Li⁺ in HTO to ion-solvent cointercalation in HTO-PA and HTO-HDA. The intercalation of large ion-solvent complexes qualitatively explains the observed further expansion of the interlayer spacing. Furthermore, this electrochemically-induced expansion is likely facilitated by the non-cross-linked structure of HTO-PA, explaining its superior kinetics compared to HTO-HDA.

Given the difficulty of analyzing the structural changes of electrode materials with reduced crystalline long-range

order during electrochemical cycling with XRD, we employ complementary electrochemical dilatometry (ECD) analysis on HTO and HTO-PA electrodes. The technique assesses the macroscopic height change of electrodes upon electrochemical (de)lithiation.[46] This allows us to verify the hypothesis of a nanoconfinement-induced cointercalation mechanism in HTO-PA. Electrochemical (de)lithiation of HTO and HTO-PA electrodes over five consecutive cycles at a rate of 50 mA g⁻¹ and the associated dilatometric responses are shown in Figure 6C–D. The significant dilatometric height change in HTO-PA is in line with previously identified cointercalation phenomena by ECD, such as the sodium-diglyme system in graphite, though smaller in absolute magnitude.[47] This can be explained by the already pre-expanded structure of pillared HTO-PA that can more readily accommodate (partially) solvated ions. It underlines that nanoconfinement-design of host materials can address the issue of excessive volumetric change of cointercalation reactions that was identified, for example, in the graphite case.[48]

With strong indications of cointercalation phenomena in HTO-PA given from the perspective of the host material response, we now employ electrochemical quartz crystal microbalance (EQCM) measurements to directly probe the nature of the (co)intercalating species in HTO-PA. The method makes use of the linear relation between the change of resonance frequency of a gold-coated quartz sensor and its mass according to the Sauerbrey equation.[49] The linearity between frequency and mass change is only valid for ideally rigid coatings on the sensor, which is why we employ a thin film coating of active material and binder by drop-casting. The dissipation of the crystal at different overtones was monitored in air, prior to cycling, to ensure the rigidity of the film. To verify the rigidity of the coating, values of changes in dissipation ΔD should be minimal and the frequency shift Δf should be independent of overtone n
<figure><img src="image_7.png" /><figcaption>**Figure 6.** Operando X-ray diffraction for (A) HTO and (B) HTO-PA, highlighting changes to the (200) plane peak over 2 consecutive cycles of galvanostatic charge and discharge at a current rate of 50 mA g⁻¹. Operando electrochemical dilatometry measurement of (C) HTO, (D) HTO-PA over 3 consecutive cycles at a current rate of 50 mA g⁻¹.</figcaption></figure>

(Figure S7).[50] We verify the rigidity of coatings in air (Figure S7A) as well as during cycling in the electrochemical cell and in contact with organic electrolyte (Figure S7B), where the condition of ΔD/Δf < 4*10⁻⁷ Hz⁻¹ is met indicating validity of the Sauerbrey equation throughout electrochemical operation.[51,52] This now allows us to investigate the mass change of the HTO-PA electrode during electrochemical intercalation via cyclic voltammetry at 0.5 mV/s (Figure 7A). Plotting of the electrode mass change against the stored charge then allows for (semi-)quantitative analysis of the intercalant. Three distinct lithiation regimes (1-3) are detected (Figure 7B). Initial lithiation occurs in the desolvated state (M<sub>w,1</sub> = 12 g/mol), coinciding with the initial shrinking detected by ECD. Subsequently, a drastic increase in the intercalant mass is detected (M<sub>w,2</sub> = 148 g/mol), indicating Li⁺ intercalation together with ca. 1.5 solvent molecules. Finally, the mass is decreased when the electrode is almost fully reduced, i.e., the interlayer space is almost

completely filled (M<sub>w,3</sub> = 68 g/mol). The similar mass of both solvents (EC and DMC) prevents us from directly identifying the involved solvent type. During delithiation, the reverse trend is observed. However, a significant hysteresis of the HTO-PA mass change of 25.6 µg cm⁻² (corresponds to 70.8% of the initial mass gain) indicates that either some solvent remains confined in the interlayer space after Li⁺ deintercalation, or the accumulation of solvent molecules at the interface of the electrode. Separating the mass changes arising from solvent accumulation at the interface and solvent cointercalation in the electrode is notoriously challenging by EQCM. Previous EQCM work on Li⁺ intercalation from EC/DMC electrolyte into TiS₂ demonstrated that solvent accumulation could lead to average molar mass changes between 20–35 g/mol,[53] which is significantly below the mass changes detected in our experiments.
<figure><img src="image_8.png" /><figcaption>**Figure 7.** EQCM measurement of HTO-PA. (A) Cyclic voltammogram of the first cycle of HTO-PA in LP30 electrolyte at a sweep rate of 0.5 mV s⁻¹, including the mass change derived from the change in resonance frequency. (B) Cumulative charge plotted versus mass change in the first cathodic cycle, with fitting of three linear regimes indicating different molar mass of the intercalant.</figcaption></figure>

A hysteresis with continued mass gain persists over the following cycles, but decreases to 50.6% and 40.7% in the second and third cycles, respectively (Figure S8). These observations also suggest that no PA pillar dissolution (which would result in mass loss) takes place over the first few cycles.

Overall, the semi-quantitative EQCM investigation demonstrates a cointercalation mechanism of partially solvated Li⁺ in HTO-PA (4 solvent molecules assumed for full solvation of Li⁺ in EC/DMC mixture[⁵⁴]). Overall, both EQCM and ECD results confirm the proposed ion-solvent cointercalation mechanism in HTO-PA, EQCM results suggest that solvent cointercalation is partially irreversible (due to mass hysteresis), but ECD results show a highly reversible swelling behavior without hysteresis. This highlights the necessity for a complete quantification of the chemical nature of the intercalant (precise solvation number and solvent type), requiring further spectroscopic analysis that must be carried out in future work.

### 3. Conclusions

A series of hydrogen titanates was synthesized that exhibits variations in (i) interlayer spacing from 0.88 to 1.58 nm and (ii) in the electrochemo-mechanical properties of the interlayer space. The variations are based on the insertion of organic pillar molecules into HTO to expand the nano-confined interlayer space, and by comparing non-cross-linking monoamine pillars (HTO-PA) with cross-linking diamine pillars (HTO-HDA). Using spectroscopic, thermogravimetric, transmission electron microscopy and diffraction experiments in combination with density functional theory, we propose optimized atomistic structural configurations of the pillared HTO materials that show consistent interlayer spacings. It was shown that linear alkyl (di)amines act effectively as pillars, because their amine group(s) form

ammonium cations that anchor to the HTO host lattice, and their alkyl backbone acts as a geometric spacer.

The electrochemical Li⁺ intercalation properties were evaluated in organic electrolyte as a function of the nano-confinement properties of the HTO host materials. It was found that interlayer expansion by molecular pillars results in an increased maximum Li⁺ storage capacity from ca. 2.1 Li⁺ per tetratitanate in pristine HTO to ca. 2.95 Li⁺ per tetratitanate in HTO-PA. The cathodic redox potential is shifted negatively by ca. 200 mV in pillared HTOs, indicating a modified electrode reaction. Moreover, the charge storage kinetics are most favorable when employing non-cross-linking PA pillars compared to cross-linking HDA pillars or pristine HTO structure, yielding a reduced charge transfer resistance and increased reversibility. Employing electrochemical operando XRD, dilatometry and EQCM, we discovered that this is due to a nanoconfinement-induced transition in intercalation mechanism from solid-solution intercalation of desolvated Li⁺ in pristine HTO to cointercalation of partially solvated Li⁺ in pillared HTO.

This work demonstrates the potential of pillared host materials to achieve electrochemical cointercalation reactions. These materials exhibit favorable thermodynamic and kinetic properties, even with standard organic electrolytes like LP30. Future work should make use of the wide design space offered by organic molecules and focus on adjustments to the pillar chemistry, e.g., replacing the alkyl backbone with polyether or aromatic molecule backbones. This has the potential to further tune and optimize the functionality of pillared host materials, in particular regarding the interaction with electrochemically intercalating ions/ion-solvent complexes.

### Acknowledgements

M.E., M.T., J.C. and S.F. acknowledge funding from the German Federal Ministry of Education and Research
(BMBF) in the “NanoMatFutur” program (grant No. 03XP0423) and financial support from the Helmholtz Association. M.E. acknowledges financial support from the Karlsruhe House of Young Scientists (KHYS) Research Travel Grant. DFT computation (H.S.; D.J.) was sponsored by the National Science Foundation (Award number: DMR-2221646). W.-Y.T. was supported by French National Agency for Research (ANR) through Chaire de Professeur Junior funding and RS2E network (STORE-EX Labex Project ANR-10-LABX-76-01). The authors thank Dr. Zenonas Jusys (HIU) for helpful discussions. Open Access funding enabled and organized by Projekt DEAL.

## Conflict of Interest

The authors declare no conflicts of interest.

## Data Availability Statement

All experimental and computational data is made available on the Zenodo repository, under DOI: 10.5281/zenodo.14258609 (https://doi.org/10.5281/zenodo.14258609).

**Keywords:** Energy storage · intercalation · layered compounds · nanoconfinement

<footnote>[1] P. Senguttuvan, G. Rousse, V. Seznec, J. Tarascon, M. R. Palacin, *Chem. Mater.* **2011**, *42*, 4109–4111.</footnote>

<footnote>[2] M. Shirpour, J. Cabana, M. Doeff, *Chem. Mater.* **2014**, *26*, 2502–2512.</footnote>

<footnote>[3] W. Yin, J. Ahn, G. Barim, J. Alvarado, M. M. Doeff, *Acc. Mater. Res.* **2024**, DOI: 10.1021/accountsmr.4c00080.</footnote>

<footnote>[4] T. K. Saothayanun, T. T. Sirinakorn, M. Ogawa, *Inorg. Chem.* **2020**, *59*, 4024–4029.</footnote>

<footnote>[5] T. Liu, L. Miao, F. Yao, W. Zhang, W. Zhao, D. Yang, Q. Feng, D. Hu, *Inorg. Chem.* **2024**, *63*, 1–26.</footnote>

<footnote>[6] H. Izawa, S. Kikkawa, M. Koizumi, *J. Phys. Chem.* **1982**, *86*, 5023–5026.</footnote>

<footnote>[7] T. Sasaki, M. Watanabe, Y. Michiue, Y. Komatsu, F. Izumi, S. Takenouchi, *Chem. Mater.* **1995**, *7*, 1001–1007.</footnote>

<footnote>[8] B. Anasori, M. R. Lukatskaya, Y. Gogotsi, *Nat. Rev. Mater.* **2017**, *2*, 16098.</footnote>

<footnote>[9] Y. Li, H. Shao, Z. Lin, J. Lu, L. Liu, B. Duployer, P. O. Å. Persson, P. Eklund, L. Hultman, M. Li, K. Chen, X. H. Zha, S. Du, P. Rozier, Z. Chai, E. Raymundo-Piñero, P. L. Taberna, P. Simon, Q. Huang, *Nat. Mater.* **2020**, *19*, 894–899.</footnote>

<footnote>[10] T. Chen, L. Xue, Z. Shi, C. Qiu, M. Sun, Y. Zhao, J. Liu, M. Ni, H. Li, J. Xu, H. Xia, *ACS Appl. Mater. Interfaces* **2022**, *14*, 54369–54388.</footnote>

<footnote>[11] Y. Zhang, E. H. Ang, Y. Yang, M. Ye, W. Du, C. C. Li, *Adv. Funct. Mater.* **2021**, *31*, 2007358.</footnote>

<footnote>[12] S. Mukherjee, C. D. Quilty, S. Yao, C. Stackhouse, L. Wang, K. J. Takeuchi, E. S. Takeuchi, F. Wang, A. C. Marschilok, E. Pomerantseva, *J. Mater. Chem. A* **2020**, *8*, 18220–18231.</footnote>

<footnote>[13] S. Saeed, S. Fleischmann, T. Kobayashi, Z. Jusys, E. Mamontov, N. C. Osti, N. P. Holzapfel, H. Song, T. Wang, S. Dai, D. Jiang, V. Augustyn, *J. Am. Chem. Soc.* **2024**, *146*, 28795–28808.</footnote>

<footnote>[14] S. Fleischmann, Y. Sun, N. C. Osti, R. Wang, E. Mamontov, D. E. Jiang, V. Augustyn, *J. Mater. Chem. A* **2020**, *8*, 412–421.</footnote>

<footnote>[15] C. Chen, N. W. Li, X. Y. Zhang, C. H. Zhang, J. Qiu, L. Yu, *Small* **2022**, *18*, 2107890.</footnote>

<footnote>[16] S. Ali, Y. Zhang, H. Yang, T. Xu, Y. Wang, J. Cui, J. E. ten Elshof, C. Shan, H. Xu, H. Yuan, *ACS Appl. Mater. Interfaces* **2023**, *15*, 5028–5037.</footnote>

<footnote>[17] L. Que, J. Wu, Z. Lan, Y. Xie, F. Yu, Z. Wang, J. Meng, X. Zhang, *Adv. Mater.* **2023**, *35*, 2307592.</footnote>

<footnote>[18] B. Jache, P. Adelhelm, *Angew. Chemie - Int. Ed.* **2014**, *53*, 10169–10173.</footnote>

<footnote>[19] Y. Sun, G. Åvall, S.-H. Wu, G. A. Ferrero, H. Wang, K. Mazzio, M. Bianchini, V. Baran, S. Risse, P. Adelhelm, *Res. Sq.* **2024**, DOI: 10.21203/rs.3.rs-4564500/v1.</footnote>

<footnote>[20] G. A. Ferrero, G. Åvall, K. A. Mazzio, Y. Son, K. Janßen, S. Risse, P. Adelhelm, *Adv. Energy Mater.* **2022**, *12*, 2202377.</footnote>

<footnote>[21] G. Åvall, G. A. Ferrero, K. A. Janßen, M. Exner, Y. Son, P. Adelhelm, G. A. Ferrero, K. A. Janßen, M. Exner, Y. Son, *Adv. Energy Mater.* **2023**, *13*, 2301944.</footnote>

<footnote>[22] H. Guo, M. Elmanzalawy, P. Sivakumar, S. Fleischmann, *Energy Environ. Sci.* **2024**, *17*, 2100–2116.</footnote>

<footnote>[23] H. Izawa, S. Kikkawa, M. Koizumi, *Polyhedron* **1983**, *2*, 741–744.</footnote>

<footnote>[24] M. Ogawa, Y. Takizawa, *Chem. Mater.* **1999**, *11*, 30–32.</footnote>

<footnote>[25] C. Airoldi, L. M. Nunes, R. F. De Farias, *Mater. Res. Bull.* **2000**, *35*, 2081–2090.</footnote>

<footnote>[26] A. A. Jeffery, A. Pradeep, M. Rajamathi, *Phys. Chem. Chem. Phys.* **2016**, *18*, 12604–12609.</footnote>

<footnote>[27] M. Piao, S. M. Oh, J. Lim, S. H. Kim, S. C. Kim, Y. K. Jo, O. H. Han, S. J. Hwang, *ACS Appl. Mater. Interfaces* **2018**, *10*, 33112–33123.</footnote>

<footnote>[28] D. Hu, L. Miao, Z. Zhang, L. Li, Y. Wang, H. Cheng, G. A. Sewvandi, Q. Feng, M. Fan, L. Zhao, *Cryst. Growth Des.* **2018**, *18*, 7264–7274.</footnote>

<footnote>[29] T. Gao, H. Fjellvåg, P. Norby, *Inorg. Chem.* **2009**, *48*, 1423–1432.</footnote>

<footnote>[30] S. Fleischmann, K. Pfeifer, M. Widmaier, H. Shim, Ö. Budak, V. Presser, *ACS Appl. Energy Mater.* **2019**, *2*, 3633–3641.</footnote>

<footnote>[31] D. Chen, M. Liu, L. Yin, T. Li, Z. Yang, X. Li, B. Fan, H. Wang, R. Zhang, Z. Li, H. Xu, H. Lu, D. Yang, J. Sun, L. Gao, *J. Mater. Chem.* **2011**, *21*, 9332–9342.</footnote>

<footnote>[32] C. Zhou, D. Wang, F. Lagunas, B. Atterberry, M. Lei, H. Hu, Z. Zhou, A. S. Filatov, D. Jiang, A. J. Rossini, R. F. Klie, D. V. Talapin, *Nat. Chem.* **2023**, *15*, 1722–1729.</footnote>

<footnote>[33] J. Karol, C. O. Ogolla, M. Dillenz, M. Sotoudeh, E. Vollmer, M. Zarrabeitia, A. Groß, B. Butz, S. Fleischmann, *ChemRxiv* **2024**, DOI: 10.26434/chemrxiv-2024-x5ggt.</footnote>

<footnote>[34] A. M. Amorim da Costa, M. P. M. Marques, L. A. E. Batista de Carvalho, *Vib. Spectrosc.* **2002**, *29*, 61–67.</footnote>

<footnote>[35] G. Tao, H. Fjellvåg, P. Norby, *J. Phys. Chem. B* **2008**, *112*, 9400–9405.</footnote>

<footnote>[36] S. H. Byeon, S. O. Lee, H. Kim, *J. Solid State Chem.* **1997**, *130*, 110–116.</footnote>

<footnote>[37] L. Qian, Z. L. Du, S. Y. Yang, Z. S. Jin, *J. Mol. Struct.* **2005**, *749*, 103–107.</footnote>

<footnote>[38] F. Jiang, Z. Zheng, Z. Xu, S. Zheng, *J. Hazard. Mater.* **2009**, *164*, 1250–1256.</footnote>

<footnote>[39] A. Jeffrey, C. Nethravathi, M. Rajamathi, *ACS Omega* **2019**, *4*, 1575–1580.</footnote>

<footnote>[40] Y. Hua, V. P. Subramaniam, D. Gong, Y. Tang, J. Highfield, S. O. Pehkonen, P. Pichat, M. K. Schreyer, Z. Chen, *J. Solid State Chem.* **2012**, *196*, 518–527.</footnote>

<footnote>[41] J. Wang, J. Polleux, J. Lim, B. Dunn, *J. Phys. Chem. C* **2007**, *111*, 14925–14931.</footnote>

<footnote>[42] V. A. Nikitina, S. Y. Vassiliev, K. J. Stevenson, *Adv. Energy Mater.* **2020**, *10*, 1903933.</footnote>

<footnote>[43] V. A. Nikitina, *Curr. Opin. Electrochem.* **2020**, *19*, 71–77.</footnote>

<footnote>[44] K. Xu, A. Von Cresce, U. Lee, *Langmuir* **2010**, *26*, 11538–11543.</footnote>
[45] Y. T. Malik, M. Braig, P. Simon, R. Zeis, S. Fleischmann, *J. Electrochem. Soc.* **2024**, *171*, 110515.

[46] I. Escher, M. Hahn, G. A. Ferrero, P. Adelhelm, *Energy Technol.* **2022**, *10*, 2101120.

[47] M. Goktas, C. Bolli, E. J. Berg, P. Novák, K. Pollok, F. Langenhorst, M. v. Roeder, O. Lenchuk, D. Mollenhauer, P. Adelhelm, *Adv. Energy Mater.* **2018**, *8*, 1702724.

[48] I. Escher, Y. Kravets, G. A. Ferrero, M. Goktas, P. Adelhelm, *Energy Technol.* **2021**, *9*, 2000880.

[49] G. Sauerbrey, *Zeitschrift für Phys.* **1959**, *155*, 206–222.

[50] N. Shpigel, M. D. Levi, D. Aurbach, *Energy Storage Mater.* **2019**, *21*, 399–413.

[51] I. Reviakine, D. Johannsmann, R. P. Richter, *Anal. Chem.* **2011**, *83*, 8838–8848.

[52] A. D. Easley, T. Ma, C. I. Eneh, J. Yun, R. M. Thakur, J. L. Lutkenhaus, *J. Polym. Sci.* **2022**, *60*, 1090–1107.

[53] J. Miranda, G. Franklin, T. S. Mathis, P. L. Taberna, P. Simon, *Energy Storage Mater.* **2024**, *65*, 103105.

[54] O. Borodin, M. Olguin, P. Ganesh, P. R. C. Kent, J. L. Allen, W. A. Henderson, *Phys. Chem. Chem. Phys.* **2016**, *18*, 164–175.

Version of record online: ■■, ■
Research Article

Layered Compounds

M. Elmanzalawy, H. Song, M. Tobis, R. Leiter, J. Choi, H. Moon, W.-Y. Tsai, D.-e. Jiang, S. Fleischmann* e202423593

Nanoconfinement-Induced Electrochemical Ion-Solvent Cointercalation in Pillared Titanate Host Materials

<figure><img src="image_9.png" /><figcaption>Modifying charge storage mechanism in HTO by organic pillars</figcaption></figure>

Interlayer-expansion of hydrogen tetratitanate is realized with organic pillars. Optimized atomistic configurations of the pillared materials are proposed by characterization with experiment and

simulation. The nanoconfinement modification of HTO induces ion-solvent cointercalation reactions with improved kinetics and increased storage capacity.