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Polarized near-infrared intersubband absorptions in CdSe colloidal quantum wells

Abstract

Colloidal quantum wells are two-dimensional materials grown with atomically-precise thickness that dictates their electronic structure. Although intersubband absorption in epitaxial quantum wells is well-known, analogous observations in non-epitaxial two-dimensional materials are sparse. Here we show that CdSe nanoplatelet quantum wells have narrow (30–200 meV), polarized intersubband absorption features when photoexcited or under applied bias, which can be tuned by thickness across the near-infrared (NIR) spectral window (900–1600 nm) inclusive of important telecommunications wavelengths. By examination of the optical absorption and polarization-resolved measurements, the NIR absorptions are assigned to electron intersubband transitions. Under photoexcitation, the intersubband features display hot carrier and Auger recombination effects similar to excitonic absorptions. Sequenced two-color photoexcitation permits the sub-picosecond modulation of the carrier temperature in such colloidal quantum wells. This work suggests that colloidal quantum wells may be promising building blocks for NIR technologies.

Introduction

Colloidal quantum wells (CQWs), often termed nanoplatelets, are a class of colloidal semiconductor materials that, in the case of zinc blende CdSe, are synthesized reliably with atomically precise control of thickness and, consequently, electronic structure1,2. CQWs are particularly attractive candidates for light-emitting applications, in which they display nearly thermally limited spectral broadening and polarized emission2,3,4,5,6,7, and as laser gain media, exhibit low-threshold, strong optical gain, and a large gain bandwidth8,9,10,11,12. These advantageous properties emerge from the interband transitions of CQWs, but the electronic structure of CQWs also naturally leads to well-defined electronic subbands13,14,15. The discretized electronic structure of epitaxial quantum wells results in narrow intersubband absorption features (between continuous subbands) in photoexcited or doped samples13,16. These intersubband absorptions have been exploited extensively in now mature infrared (IR) technologies, such as quantum cascade lasers and IR detectors17,18,19, and they have been proposed for use in ultrafast all-optical switching20,21.

Substantial efforts to fabricate thinner epitaxial quantum well structures using wider bandgap semiconductors have extended the energy range of intersubband absorption to the near-IR (NIR)22,23,24,25,26,27, which is particularly coveted for use in telecommunications windows at 1.3 and 1.55 μm wavelengths. However, generation of narrow intersubband absorption resonances in the NIR remains a challenge for epitaxial quantum wells both due to inhomogeneity of the growth process and strain or defects introduced at interfaces. Related to intersubbands observed in quantum wells, intraband absorptions between discreet states have been observed in colloidal28 and epitaxial quantum dot systems29, but these are in the mid-IR. Recent advances in materials science have created several new classes of materials, which display a quantum well-like electronic structure but do not require epitaxial growth, including van der Waals two-dimensional materials (which have reported mid-IR intersubband absorptions)30, quasi-two-dimensional perovskites31, and CQWs2.

Here, intersubband absorptions are realized in CdSe CQWs of 3.5–6.5 monolayers (MLs are defined as atomic units of Cd and Se; CQWs terminate with cadmium on both large faces making a half layer) spanning the NIR spectral range. By definition CQWs do not require epitaxial growth but they still form atomically sharp interfaces with organic ligand coatings and core/shell heterostructures. Coupled to the synthesis of ensembles with monodisperse thickness2,9,32, intersubband absorptions of CQWs are spectrally narrow (30–200 meV) and tunable from 900 to 1600 nm for examined samples. Comparison of photoinduced absorptions and spectroelectrochemical data with static absorption spectroscopy and polarization-resolved measurements confirm that the NIR features are attributable to intersubband absorptions of electrons from the first to second electron subbands. Similar to band-edge absorptions, photo-induced intersubband absorptions in CQWs show multiexcitonic physics and carrier thermalization effects on dynamics and spectra. Last, this work demonstrates that intersubband absorption features can be exploited for sub-picosecond optical modulation.

Results

Polarized NIR-induced absorptions of CQWs

Typical static absorption spectra of CdSe CQWs are shown in Fig. 1a (transmission electron microscopy is shown in Supplementary Fig. 1.) CdSe CQWs are transparent in the NIR and show excitonic absorptions at visible wavelengths determined by their two-dimensional electronic structure. The excitonic wavelengths are diagnostic of the CQW thickness, here shown for 3.5 to 6.5 ML samples. Thinner or thicker CQWs of CdSe33,34 or other compositions2 (e.g., CdS or CdTe) are anticipated to show similar phenomena to the following, but there is currently less synthetic control over those compositions. Upon absorption of an above-bandgap photon, the CQWs display three bleaching features, shown in Fig. 1b, which represent heavy-hole (HH), light-hole (LH), and spin–orbit (SO) hole transitions to the first electronic shelf (E1)2. At the same time, and displayed in Fig. 1c, spectrally narrow absorption features emerge in the NIR spectral window. Similar NIR-photoinduced absorptions have been reported once before35, but in that case they were attributed to an unspecified process, which roughly tracks the energy of the HH transition. In a recent report on the properties of PbSe/CdSe dot-on-plate heterostructures, NIR-photoinduced absorptions are also observed, but not addressed directly36. The energetic position of the NIR absorption features depends on the CQW thickness: identical photoinduced absorptions were observed in other CQW samples with the same thickness. The energy of the NIR feature red-shifts for thicker CQWs and particularly noteworthy are the photoinduced absorption features of the 5.5 and 6.5 ML samples, which appear at the 1.3 and 1.55 μm bands used in telecommunications. Based on a comparison of the visible bleach feature with the strength of the NIR absorption, the oscillator strength of the NIR absorptions are approximately one-fortieth (i.e., 10−15 to 10−16 cm−2) of the band-edge absorption resonances, which depend strongly on lateral area37.

Two additional experiments support that the NIR-photoinduced absorptions arise from intersubband transitions. First, the kinetics of the visible bleaching feature and the NIR-induced absorption were directly compared for the same samples at similar pump fluence. As shown in Fig. 1d, the kinetic traces of these features overlap for each of the samples measured, which provides evidence that the NIR-photoinduced absorption occurs when excitons are present in the nanostructures. Second, spectroelectrochemical results demonstrate that NIR absorption features are obtained for CQW films when electrochemically charged. Solid thin films of CQWs are prepared by drop-casting followed by soaking for 1 min in a 5 mg mL−1 methanolic solution of benzoic acid. Similar to earlier reports on electrochromic quantum dots38, negative applied biases lead to filling of the CdSe CQW conduction band with electrons, which reveals intersubband absorption features of electrons (Fig. 1e). The conductivity of the CQW films also increases as electrons fill the conduction band (Supplementary Fig. 2). As plotted in Fig. 1e, the NIR-induced absorption features observed in spectroelectrochemical experiments are nearly identical in energy to those observed after photoexcitation. These experiments indicate that CQWs display intersubband absorptions of electrons in the conduction band with energies dictated by the CQW thickness.

To assign the specific transition responsible for the NIR-induced absorption feature, the electronic structure of the CQWs is illustrated in Fig. 2a with transitions of a 6.5 ML CQW sample. CQWs’ electronic structure consists of electron and hole states with quantum number subscripted n; hole states split into HH, LH, and SO bands. The three lowest-energy static absorption features are identified as HH1, LH1, and SO1 transitions to the E1 state, respectively2. The fourth and fifth transitions observed in the optical spectrum are identified as HH2 and LH2 band transitions to the second electronic shelf of the conduction band (E2), consistent with effective mass models of the energetic spacing (Supplementary Fig. 3) and in keeping with the fact that the strongest interband transitions of quantum wells have the same quantum number33,39.

An additional factor that complicates the interpretation of the absorption spectrum of CQWs is the exciton binding energy, which reduces the energy of the observed optical resonances with respect to the band positions. Each interband (quantum number n) transition of the CQWs has a distinct exciton binding energy, denoted $$E_{\mathrm{b}}\left[ {{\mathrm{HH}}_n \to E_n} \right]$$ for the HH to electron band transitions. Therefore, the energy differences of electron and hole bands of different quantum numbers are not directly accessible from absorption measurements both due to selection rules of interband transitions (Δn = 0 rule) and exciton binding energy effects. Given the evidence that the NIR-induced absorption feature reflects an intersubband absorption of electrons, and compared with spectroscopic evidence in Fig. 2b, the main interssubband absorption for electrons in a wide-gap material such as CdSe is expected to be for the E1 → E2 transition. This transition is allowed, with strong expected polarization, addressed below40,41,42. A more complete derivation may be found in the Supplementary Information, but due to these two adjustments, the energy of the first electron intersubband absorption can be estimated from absorption spectra as

$$E\left[ {E_1 \to E_2} \right] = \left( {E\left[ {{\mathrm{HH}}_2 \to E_2} \right] - E\left[ {{\mathrm{HH}}_1 \to E_1} \right]} \right) \\ - \left( {E\left[ {{\mathrm{HH}}_1 \to {\mathrm{HH}}_2} \right] + E_{\mathrm{b}}\left[ {{\mathrm{HH}}_1 \to E_1} \right] - E_{\mathrm{b}}\left[ {{\mathrm{HH}}_2 \to E_2} \right]} \right),$$
(1)

which takes into account the energy of optically allowed interband and intersubband transitions, indicated with arrows as, for example, $$E\left[ {E_1 \to E_2} \right]$$, and the exciton binding energies of interband transitions, indicated as for example, $$E_{\mathrm{b}}\left[ {{\mathrm{HH}}_1 \to E_1} \right]$$. In this case, because hole intersubband transitions are not observed, and the exciton binding energies of the relevant interband transitions are inexactly defined, the problem is underdetermined. The experimentally observed energy difference between interband transitions denoted $$\left( {E\left[ {{\mathrm{HH}}_2 \to E_2} \right] - E\left[ {{\mathrm{HH}}_1 \to E_1} \right]} \right)$$ represents an upper limit on the energy of electron intersubband transition. A similar argument applies to the hole intersubband transitions.

Figure 2b shows this empirical upper energy limit and the energy positions of experimentally observed NIR intersubband absorptions, which fall below this empirical upper limit. The gaps is 513, 322, 262, and 209 meV for 3.5, 4.5, 5.5, and 6.5 ML CQWs, respectively. This is consistent with the additional energy $$E\left[ {{\mathrm{HH}}_1 \to {\mathrm{HH}}_2} \right]$$ necessary for the first HH intersubband transition and differences in the exciton binding energy of the respective interband transitions ($$E_{\mathrm{b}}\left[ {{\mathrm{HH}}_1 \to E_1} \right] - E_{\mathrm{b}}\left[ {{\mathrm{HH}}_2 \to E_2} \right]$$), both of which decrease for thicker CQWs. The precise contribution of the hole transitions and the differences in exciton binding energies is not known. Given available estimates of the exciton binding energy $$E_{\mathrm{b}}\left[ {{\mathrm{HH}}_1 \to E_1} \right]$$, a lower limit for the higher exciton binding energies may be estimated with a Rydberg model for two-dimensional hydrogenic excitons as $$E_{\mathrm{b}}\left( n \right) \propto \left( {n - 1/2} \right)^{ - 2}$$, although the accuracy of this model is questioned in other two-dimensional materials43. This estimate suggests a reduction in the exciton binding energy from the $$E_{\mathrm{b}}\left[ {{\mathrm{HH}}_1 \to E_1} \right]$$ to $$E_{\mathrm{b}}\left[ {{\mathrm{HH}}_2 \to E_2} \right]$$ by roughly a factor of 10, which places the differences of the exciton binding energies of the first and second interband transitions at 90–360 meV.

As noted above, in epitaxial quantum wells, it is well known that the E1 → E2 intersubband transition is highly polarized in the short axis of the wells18. Photoselection anisotropy transient absorption can therefore confirm the E1 → E2 intersubband transition. Measurements of photoselection anisotropy using transient absorption are similar to fluorescence anisotropy measurements, except that in transient absorption, both excitation and probe dipoles relate to the absorption. A polarized excitation source (350 nm laser) photoselects a subset of the ensemble for which the absorption dipole is aligned with the excitation, then the sample is examined with parallel or perpendicular polarized probe beams. Polarization-resolved transient absorption spectra for the NIR features at a delay of 10 ps of CQWs are shown in Fig. 3a–d. In each case, the induced absorption feature is stronger in the polarization perpendicular to the pump beam. An isotropic sample of lead selenide quantum dots in Supplementary Fig. 4 confirms that the experimental setup is not the origin of the observed polarization effects. Unlike molecular systems, large CQWs do not undergo rotational depolarization on the measurement time-scale (Supplementary Fig. 5).

The intensity ratio of the photoinduced absorptions (or visible bleaches) is determined by the axes of the CQWs on which different excitations occur. The measured transient absorption anisotropy of an isotropic ensemble is

$$R = \frac{{\Delta \alpha _\parallel - \Delta \alpha _ \bot }}{{\Delta \alpha _\parallel + 2\Delta \alpha _ \bot }} = \frac{2}{5}r_{{\mathrm{pump}}}r_{{\mathrm{probe}}},$$
(2)

in which ri is the anisotropy of the pump and probe wavelength intensity (I)44. For arbitrary isotropic ensembles, the range of anisotropy is from −0.2 to 0.4; assuming, as is reasonable in this case, that the two-dimensional plate of the CQW has degenerate long axes (x, y), ri is $$I_{zi} - I_{xi,yi}/I_{zi} + 2I_{xi,yi}$$ with respect to the fluorophore axes, where the intensities may be normalized such that $$I_x + I_y + I_z = 1$$. When pump and probe absorption dipoles are exclusively in-plane ($$I_{x} = I_{y} = 0.5$$), the anisotropy is 0.1, which is indeed close to the anisotropy measured for the visible bleach features of the CQWs (Supplementary Fig. 6). This is also consistent with many previous works showing that interband transitions of CQWs are in-plane5,6,45,46. Non-idealities, like rectangular in-plane shape or bending and twisting of the CQWs—more prominent in thinner CQWs47—may impose some deviations from this idealized picture. Returning to Fig. 3e, the anisotropy values measured at the intersubband absorption are negative, with values reaching as low as −0.18. These results may only be achieved when the pump absorption dipole is polarized almost exclusively in-plane, but the probe absorption dipole is polarized almost exclusively in the unique out-of-plane axis as shown in the cartoon in Fig. 3f. Given that this is precisely what is observed in epitaxial quantum wells for the E1E2 transition, polarized measurements support the assignment of the NIR-induced absorption features to the E1E2 intersubband transition of the CQWs.

Temperature-dependent intersubband absorption

The samples were additionally examined by temperature-dependent spectroscopy to ascertain the change in bandwidth and energy of the intersubband absorption features. Figure 4a–c show temperature-dependent photoinduced absorption, and with corresponding static absorption spectra of 4.5, 5.5, and 6.5 ML samples in Fig. 4d–f. Both intersubband and interband transitions red-shift at higher temperatures due to lattice expansion. Figure 4g plots the energy and bandwidth of the NIR intersubband absorption features as a function of temperature for the 4.5, 5.5, and 6.5 ML samples. Over the studied temperature range, the intersubband absorptions shift linearly with a thermochromic coefficient of −1.9 × 10−4, −1.4 × 10−4, and −9.9 × 10−5 eV/K for 4.5, 5.5, and 6.5 ML CQWs, respectively, which are somewhat smaller than reported values of the Varshni α term for the temperature-dependent band gap change of CdSe nanocrystals and CQWs48,49,50,51,52,53,54,55.

The bandwidth of the intersubband absorption feature (like interband absorptions) is temperature-sensitive due to the increased electron–phonon coupling that also influences the ensemble linewidths of the band-edge transitions2,52,56. For example, the 6.5 ML CQW intersubband absorption narrows from 70 to 34 meV full-width at half-maximum at 450 and 80 K, respectively. A pronounced asymmetry for the 6.5 ML CQW sample at high temperature is most likely due to poor linearity of the InGaAs array detector response for wavelengths >1575 nm. By comparison, intersubband absorption features in GaN/AlN epitaxial quantum wells of comparable energy (corresponding to c. 1.55 μm) show full-widths at half-maximum energies of 160 meV or greater20,23. Although intraband absorptions in zero-dimensional quantum dots can be similarly narrow, they typically have energies <500 meV. Interband transitions of mercury chalcogenide CQWs show line width of the absorption and photoluminescence features of 60 meV at room temperature at close to 900 nm57, which is narrower than the 3.5 ML CdSe CQW intersubband absorption and comparable to 6.5 ML CQWs under photoexcitation; however, the energy range of these interband transitions is presently limited.

Figure 4h displays the empirical upper energy limit ($$E\left[ {{\mathrm{HH}}_2 \to E_2} \right] - E\left[ {{\mathrm{HH}}_1 \to E_1} \right]$$) of the E1 → E2 intersubband transition at many temperatures, calculated from the optical absorption spectra. $$E\left[ {{\mathrm{HH}}_2 \to E_2} \right] - E\left[ {{\mathrm{HH}}_1 \to E_1} \right]$$ exceeds the observed intersubband transition energy for all thicknesses of CQW and all temperatures (Fig. 2b), due to hole intersubband transitions and exciton binding energy differences. Indeed, this energy gap is nearly constant with temperature for a given thickness of CQW, as demonstrated in Fig. 4i.

Fluence-dependent effects on intersubband absorptions

Similar to excitonic absorptions of semiconductor nanocrystals, the intersubband absorptions of the CQWs display fluence-dependent Auger and hot-carrier effects. With higher pump fluences at early delay times, the strength of intersubband absorption increases (shown in Fig. 5a for a 5.5 ML CQW sample), but sub-linear growth is observed at the highest examined fluence as the CQW exciton transition saturates. Elevated pump fluences also initiate multiexciton physics, chiefly Auger recombination, which dramatically changes the kinetics of the intersubband induced absorption. Similar to other semiconductor nanomaterials, Auger recombination manifests as an accelerated decay of the Δα signal, as shown in Fig. 5b, above the fluence threshold (here >10 μJ/cm2) that generates more than one electron–hole pair per CQW58,59. For the 5.5 ML CQW sample studied in Fig. 5, the biexcitonic Auger time estimated from fluence-dependent kinetics of the intersubband photoinduced absorption is 225 ± 50 ps, which is comparable to previous measurements based on time-resolved photoluminescence9.

Hot-carrier effects on the intersubband absorption features are chiefly dictated by the presence or absence of multiexciton Auger recombination, displaying distinct behavior based on the incident fluence. Fluence-dependent hot-carrier effects are well known in bulk materials60, epitaxial quantum wells61, and even CQWs35, but explicit spectroscopic investigations of the influence of hot carriers on intersubband resonances in epitaxial quantum wells are limited to demonstrations of line broadening62. At low fluences, as in Fig. 5c, the signature of hot-carrier absorption is the broadened and red-shifted photoinduced absorption, which decays within <2 ps to the spectrum observed at long delay times. Unlike electronic bleaches or photoluminescence, for which hot-carrier effects are manifest from blue-shifted spectral signatures at the band edge, the intersubband absorption predominantly shows a red-shift because the energy difference between the E1 and E2 bands effectively decreases for hot carriers in the E1 band. The specific nature of intersubband transition broadening for hot carriers also depends on the non-parabolicity of the bands. Under high fluence conditions, as shown in Fig. 5d, thermal relaxation of carriers observed via the intersubband absorption is spectrally apparent from the broadened response for at least 100 ps after the excitation pulse, chiefly arising from continuous heating of electrons due to Auger recombination, although lattice heating may also play a role on such time-scales35.

Optical switching with intersubband transitions in CQWs

Intersubband transitions in epitaxial quantum wells have long been viewed as promising candidates for optical switching technologies21,63,64, in addition to their extensive use in quantum cascade lasers and IR detectors. Primarily, this is because excitation of carriers within subbands typically results in sub-picosecond relaxation, particularly compared with interband processes (e.g., up to 50 ns in 900 nm band-edge HgTe CQWs57) or even intraband relaxation in quantum dots (e.g., many picoseconds in CdSe quantum dots65). Whereas optical excitation can produce an add/drop switch with appearance and decay of the NIR absorption feature, to create a faster optical switch using intersubband absorptions of CdSe CQWs, which have no static intersubband absorption in their as-synthesized state, two pump excitations are used. First, an unchopped above-band-gap blue excitation (400 nm) is used to excite the sample and generate an intersubband absorption resonance shown in Fig. 6a. The second, chopped, IR pump pulse is delivered at a delay of 50 ps (after cooling of carriers), with the center wavelength of such pulses tuned near the intersubband absorption feature. Transient spectra were collected in the visible near the band-edge absorption features by comparing the IR pump on vs. IR pump off signals. The fluence of the IR pump pulse was maintained sufficiently low for all wavelengths (c. 500 μJ/cm2) that multiphoton absorption and concomitant state filling was not observed experimentally, as shown in Fig. 6b. The transient signal near the band-edge HH to E1 transition represents the dynamics of heating and cooling of electrons in the conduction band of CQWs.

The IR re-pump pulse closest to the intersubband absorption resonance generated the largest induced absorption feature at red side of the CQW band-edge absorption feature. However, off-resonance wavelengths also result in transient induced absorption, most likely by exciting the weaker, but continuous photoinduced absorption arising from intraband transitions of photoexcited carriers. The positive sign of the Δα signal (induced absorption) is expected on the red edge of the band-edge absorption feature: exciting carriers in the E1 band of the CQWs transiently heats those carriers above ambient temperature, reducing their occupation of the E1 band edge and permitting increased absorption until carriers cool back to ambient temperature. Cooling back to room temperature occurs with an exponential lifetime of 530 fs, determined by fitting the decay kinetic with 1260 nm IR re-pump (see Supplementary Fig. 7).

Discussion

CdSe CQWs display photoinduced or charging-induced absorption features at wavelengths spanning 1550 nm for 6.5-ML-thick CQWs to 900 nm for 3.5-ML-thick CQWs at room temperature. A combination of detailed analysis of static optical spectra, dynamics, and polarized spectroscopy confirms that the observed transitions are intersubband transitions of electrons from the first electronic shelf to the second electronic shelf of the CQWs. This observation maps well on to the band structure models developed for epitaxial quantum wells, as has already been found for interband transitions, but with the distinct advantages emergent from colloidal synthesis, such as scalability and lifting of epitaxial constraints. Recent synthetic work to expand the range of CQWs available to thinner and thicker sizes32,33,34 may further expand the range of intersubband transitions into the MIR and visible. The narrow spectral bandwidth of the intersubband absorptions in CQWs compared to epitaxial systems is particularly noteworthy. Recent work showing the critical role of surface termination on the lattice strain of CQWs, CQW band gap, and CQW transition line widths underlines the potential of colloidal systems to relax to a state with reduced bandwidth compared to epitaxial systems66,67,68. In the future, this can be explicitly explored with atomically precise epitaxial interfaces.

These results convey that many related systems, which have similar electronic structure, such as CQWs of other compositions, two-dimensional van der Waals quantum wells, or quasi-two-dimensional perovskite materials, are also likely to show similar intersubband absorptions. Previous investigations of these van der Waals structures, in particular, have already demonstrated intersubband transitions in the mid-IR30. Variation of composition to achieve larger band gaps, which are typically accompanied by larger subband spacings, and greater asymmetry of carrier effective masses are likely to drive such intersubband transitions to higher energy. Controlled doping and self-assembly of CQWs may enable NIR technologies analogous to those of epitaxial quantum wells, such as detectors and multiwell light-emitting technologies.

Methods

Materials

Cadmium acetate hydrate (≥99.99%, Aldrich), cadmium chloride (99.99%, Aldrich), hexanes (99.9%, Fisher), methylcyclohexane (≥99%, anhydrous, Aldrich), selenium (99.99%, powder, ~100 mesh, Aldrich), 1-octadecene (90%, technical grade, Aldrich), oleic acid (90%, technical grade, Aldrich), cadmium nitrate (97%, Aldrich), tetrabutylammonium perchlorate (>99.0%), benzoic acid (99.5%, Aldrich), and sodium myristate (>98%, Aldrich) were sourced from commercial suppliers and used as received. Solvents used were sourced from commercial suppliers and were ACS grade or higher.

Synthesis

Room temperature static absorption spectra of methylcyclohexane solutions were collected using a Cary 50 UV–Vis spectrometer. Temperature-dependent measurements were made on solid films drop-cast from methylcyclohexane on to sapphire windows using a deuterium halogen lamp focused through the samples mounted on sapphire in a nitrogen-cooled cryostat and detected using an Ocean Optics spectrometer. Room temperature solution NIR measurements were performed using a Nicolet 6700 FT-IR (Fourier transform infrared) with an InGaAs detector with samples dispersed in carbon tetrachloride in quartz cuvettes.

Microscopy

Transmission electron microscopy images of CQW samples were collected using a JEOL 2100F microscope operated at 200 keV.

Time-resolved spectroscopy

Transient absorption data was collected using Ultrafast Systems equipment operating at either 5 kHz (~100 fs pulses) or 2 kHz probe frequency (~35 fs pulses), with alternate pump shots blocked with a mechanical chopper. Methylcyclohexane dispersions in 1 mm quartz cuvettes with a band-edge optical density of ~0.5 were used for experiments at room temperature, although the response of solid films on glass or sapphire were not substantially different. For temperature-dependent measurements, solid films were prepared by drop-casting methylcyclohexane dispersions on to a sapphire window to achieve a similar optical density. For polarization-sensitive measurements, a linear polarizer was placed after the sample to select parallel and perpendicular components of the white probe light. The strength of different polarizations of the probe light was adjusted to achieve similar intensities with both polarizations by adjusting the relative angle of the sapphire crystal used to generate the white light compared to the driving 800 nm pulse. For two-pump pulse measurements, the experiment was first configured to obtain mutually overlapping spots of the NIR and blue (400 nm) pump beams and the probe beam, with the two pump beams separated by ~50 ps in time. Overlap of the NIR beam was initially performed at high fluence to induce multiphoton absorption. (Multiphoton absorption can also induce the same intersubband absorptions.) To isolate dynamics associated with the IR pump pulse on a photoexcited sample, the 400 nm pump beam was unchopped (2 kHz) and the IR pump pulse was chopped at 1 kHz.

Spectroelectrochemistry

Spectroelectrochemistry was performed similar to an earlier work69. Samples were prepared by drop-casting CQWs dispersed in methylcyclohexane (optical density at band-edge exciton >3 cm−1) on to gold interdigitated electrodes designed for a home-built spectroelectrochemical cell. Thin films were ~200 nm thick, estimated from optical absorption. Measurements were performed using a Nicolet S50 FT-IR. The drop-cast thin films were treated in air with a 5 mg mL−1 benzoic acid solution in methanol for 1 min, washed in air by immersion in clean methanol solutions three times for 30 s, and then blown dry with nitrogen. The film coverage of the electrodes varied substantially after this processing due to delamination during the washing steps. The electrolyte was 0.1 M tetrabutylammonium perchlorate in dried and degassed propylene carbonate and the sample cell was loaded in a nitrogen glovebox to minimize oxygen contamination For each measurement at a new voltage, a background at −0.044 vs. saturated calomel electrode was first collected and the current measured between the interdigitated electrodes was allowed to stabilize (typically within 3 min) before starting the FT-IR measurement. Using the interdigitated working electrodes, conductance of the channel was also measured at various applied potentials. Potentials of data presented in the work were chosen to achieve adequate signal to noise and do not reflect the minimum sufficient voltages of band filling for the samples.

Data availability

All source data are available from the authors.

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Acknowledgements

M.C. and I.C. were supported by the University of Chicago Materials Research Science and Engineering Center, which is funded by the NSF under award number DMR-1420709. This work was performed, in part, at the Center for Nanoscale Materials, a US Department of Energy Office of Science User Facility, and supported by the US Department of Energy, Office of Science, under Contract No. DE-AC02-06CH11357. We acknowledge support from the NSF DMREF Program under awards DMR-1629383 and DMR-1629601.

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B.T.D. and R.D.S. conceived and executed optical experiments. B.T.D. and M.C. performed spectroelectrochemistry experiments. B.T.D., I.C., and K.R.W. performed syntheses. R.D.S, D.V.T., and P.G.-S. supervised work. All authors contributed to writing the manuscript.

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Correspondence to Benjamin T. Diroll or Richard D. Schaller.

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Diroll, B.T., Chen, M., Coropceanu, I. et al. Polarized near-infrared intersubband absorptions in CdSe colloidal quantum wells. Nat Commun 10, 4511 (2019). https://doi.org/10.1038/s41467-019-12503-z

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