Abstract
SuperPlanckian nearfield radiative heat transfer allows effective heat transfer between a hot and a cold body to increase beyond the limits long known for black bodies. Until present, experimental techniques to measure the radiative heat flow relied on steadystate systems. Here, we present a dynamic measurement approach based on the transient plane source technique, which extracts thermal properties from a temperature transient caused by a step input power function. Using this versatile method, that requires only single sided contact, we measure enhanced radiative conduction up to 16 times higher than the blackbody limit on centimeter sized glass samples without any specialized sample preparation or nanofabrication.
Introduction
In the far field, the electromagnetic radiation emitted by a hot body is limited to the wellknown blackbody distribution originally derived by Planck^{1}. However, this theory is only valid when the characteristic dimensions of the body are significantly greater than the wavelength of maximal thermal radiation, ~10 µm at 300 K. When bodies at different temperatures do not satisfy this criterion, then the radiative heat flux may display drastically different characteristics. Particularly, if the separation distance is smaller than the maximum wavelength the radiative heat flux can be orders of magnitude greater than the blackbody limit, a phenomenon known as nearfield radiative heat transfer (NFRHT)^{2,3}. This results from the contribution of tunneling (evanescent) thermal photons associated with large tangential wave numbers across the vacuum gap separating the bodies. The smaller the separation distance is, the greater the contribution of these decaying modes and, consequently, the higher the heat flux^{2,3,4}.
Given its importance as a generalization of Kirchhoff law of thermal radiation, NFRHT has garnered considerable scientific interest, spanning computational aspects^{4,5,6}, the effect of surface^{7,8} and hyperbolic modes^{9,10,11,12,13}, and potential applications^{14,15,16,17,18}. A number of experiments demonstrating NFRHT in different geometries have also been reported, each with their own merits and drawbacks. Tipplane^{19,20,21,22,23,24,25,26,27} and sphereplane^{28,29,30,31,32,33,34,35,36} geometries allow for surface mapping and precise distance control, but suffer from complicated data analysis. Planeplane experiments offer the advantage of simple interpretation and large, easily detectable, heat fluxes^{14,37,38,39,40,41,42,43,44,45,46,47}, however, these experiments are complicated by the need to create uniform submicrometer gaps. Other geometries combine advantages of these geometries, but suffer from their own challenges, such as elaborate microfabrication of samples^{48,49}.
While the details of these experiments are widely varied, they are tied by a single, dominant, operational paradigm: One side is heated with constant power, and the other is kept at constant lower temperature. The temperatures on hot and cold sides, along with heat power flux, are then measured once the system has reached a steady state (stationary), and from these quantities the nearfield heat conductance – radiative heat power flux normalized to the temperature difference – is determined. That is, these experiments are all performed under stationary (steadystate) conditions, where by “stationary” we refer to nontimevarying systems. “Steadystate” measurement techniques allow variations at one frequency (and its harmonics), thus include “stationary” measurements, but forbid the measurement of any transient effects. In some of the NFRHT experiments the gap size^{14,19,20,24,36,46} or the heating power^{25,36,46} is modulated to improve sensitivity. Yet even in these cases, measurements are conducted only once steadystate conditions have been achieved, and the measured quantities directly determine the gap conductance.
In theory, this is the simplest (most straight forward and indisputable) method of measuring the power transferred by thermal radiation. However in practice, there are a number of drawbacks:

(I)
All other resistances and losses between the sensors must be carefully approximated or eliminated before the gap conductance can be measured.

(II)
The sensors and heaters/coolers must be built into the system. This requires sample accessibility from both sides of the gap where thermal heat transfer is taking place, and good contacting. Often, additional micro/nanofabrication steps are utilized for that.

(III)
The time for an object to thermalize is approximately \( \sim \,{R}^{2}/\alpha \), with \(R\) standing for the largest characteristic length, and α the thermal diffusivity. If a sample has any characteristic dimensions on the centimeter scale then it can quickly become very time consuming – several minutes to several tens of minutes – to wait for thermal transients to decay.
Here, we report a dynamic NFRHT measurement procedure based on the transient plane source (TPS) technique^{50,51} that substantially alleviates these functional concerns. Notably, the approach requires no specialized sample preparation or microfabrication steps. We present experimental data showing the viability of our method using centimeter sized samples consisting of two optical glass disks separated by gaps varying from 7 µm down to 150 nm. This data agrees precisely with expected theoretical values, and marks the highest radiative thermal conductance enhancement, up to 16 times greater than the blackbody limit, reported for such macroscopic samples. Further, our method requires only one side of the sample to be contacted, and provides additional information about the thermal dynamics of the sample not measurable with stationary approaches. Conceivably, it also allows for the resolution of thermal conductance at multiple gaps; and provides a vital step towards analyzing and implementing systems making use of dynamic thermal effects in the near field.
Methods
Transient plane source (TPS) technique
The basis of our technique is the transient plane source (TPS) method, commonly used in the determination of bulk thermal parameters. In this approach, a thin disk consisting of a nickel double spiral embedded in Kapton^{52,53} insulation, acts both as a heat source and temperature sensor. To perform a measurement, the sensor/heater is brought into contact with the material under investigation, and a step power input function is applied. The temperature transient is then recorded by measuring the changing resistive load of the sensor/heater which is then a function of the heat conductance of the environment with which the sensor/heater is in contact.
The thermal properties, including any potential boundary effects, of the surrounding material influence the shape of this temperature transient. As each bulk thermal characteristic affects heat transport in a distinct way, the transient contains enough information to simultaneously extract thermal conductivity and diffusivity without knowledge of the specific heat capacity^{50,51}. (Our measurements have been conducted using a commercially available TPS 2500 S from Hot Disk AB, and a Kapton sensor/heater of 19.8 mm diameter provided by this same company). To our knowledge, the here presented work is the first extension of the TPS technique to nearfield measurements.
NFRHT measurements
Our nearfield measurements are carried out using interferometric quality BK7 and fused silica glass disks with 20 mm diameter and 5 mm height. To create and maintain a gap between the lower disk (substrate) and upper disk (superstrate), monodisperse silica micro/nanospheres are used as spacers^{39}. The gap size is then confirmed by interferometric reflectivity measurements^{43,44}. Once prepared, the gap setup is placed onto the TPS sensor/heater using thermal paste (Apiezon L Grease from M&I Materials Ltd) to improve the sensor/heatersubstrate contact. (A detailed explanation of the sample specifications and preparation procedures is presented in Supplementary Information S1. Additional information on gap size measurements is presented in Supplementary Information S6).
To mitigate both convective and conductive heat flow from the boundaries, the sample and sensor/heater are then placed in a vacuum chamber (reaching a pressure of approximately 10^{−5} mbar). Two measurements are performed. First, the temperature transient of the gap sample is measured without modification. Next, the superstrate is carefully taken away such that the setup remains otherwise unchanged, Fig. 1. This second measurement serves as a reference, thus, this sample is called the reference sample. For both measurements, a power input of 40 mW is applied to the sensor/heater for 640 s. In Fig. 3 two examples of measured gap transients for gap sizes of 315 nm and 2.75 µm are shown for BK7 and for fused silica along with their reference transients. When the glass superstrate is present, nearfield radiative heat transfer allows additional heat to escape the substrate, lowering its temperature at constant heating power (Fig. 1 inset). The smaller the gap the stronger this effect is. Note that the transients begin to differ significantly only once the heat front originating from the sensor/heater has reached the upper surface of the substrate, confirming the validity of the reference.
1D model and fitting
As the measurement is dynamic, the thermal conductance of the gap cannot be read out directly. Rather, this information must be extracted from the shape of the transient by a fitting procedure. To accomplish this fitting, we utilize two models; a simple 1dimensional (1D) stack and a more comprehensive, hence complex, 2dimensional (2D) finitedifferencetimedomain (FDTD) gaped cylinder^{54,55}.
The framework of the 1D model is illustrated in Fig. 2. The glass disks serving as substrates and superstrates are divided into N layers, each with a thermal capacity \(m{c}_{1/2,j}\), and a relative temperature \({\rm{\Delta }}{T}_{1/2,j}\) with respect to the thermal equilibrium temperature \({T}_{0}\) = 294 K (±1 K). N1 resistances \({R}_{1/2,j}\) separate these layers, comprising the thermal resistivity of the disks. Additionally, the TPS sensor/heater has a capacity \(m{c}_{sen}\) and temperature \({\rm{\Delta }}{T}_{sen}\) and the gap as well as the sensor/heatersubstrate contact are represented as resistances \({R}_{gap}\) and \({R}_{c}\). At \(t\) = 0 heat with a power of \({P}_{in}\) = 40 mW is applied to the sensor/heater. As time progresses, this input power to the sensor/heater is countered by conductive and radiative losses to the base and radiative losses to free space. We model these additional effects as the conductance \({h}_{sen}\) and emissivities \(\varepsilon \), assuming linear dependence on \({\rm{\Delta }}T\). The validity of this assumption rests on the fact that \({\rm{\Delta }}T\) is small compared to \({T}_{0}\), and is one of the reasons a small input power is used. This 1D model provides an analytic solution for the layer temperatures as a function of time, including the sensor/heater temperature. The equations as well as parameter values are given in Supplementary Information S5. Further, the underlying assumptions of 1dimensionality and linear response are verified by a more comprehensive finite difference model (2D FDTD model).
The fitting procedure proceeds as follows: First, we fit the reference sample measurements; determining the contact resistance \(\,{R}_{c}\), top emissivity \({\varepsilon }_{top}\), side emissivity \({\varepsilon }_{side}\) (we assume all side emissivities to be equal \({\varepsilon }_{1/2,j}={\varepsilon }_{side}\,(\forall j)\)), and sensor/heater loss conductance \({h}_{sen}\). (\({\varepsilon }_{top}\) and \({\varepsilon }_{side}\) are identical for all BK7 references and all fused silica references.) \({R}_{c}\) and \({h}_{sen}\) vary from measurement to measurement as the sensor/heatersubstrate contact is intrinsically variable due to varying thickness and morphology of the thermal paste layer used to contact the sensor/heater to the glass disk and due to small differences in the position where the sensor/heater lies on the insulator. The fitted figures are \({\varepsilon }_{top}={\varepsilon }_{side}\) = 0.85 for BK7 and \({\varepsilon }_{top}={\varepsilon }_{side}\) = 0.89 for fused silica. Note that these fits were compared against absorptivity measurements from a Fourier Transform Spectrometer (FTIR) (VERTEX 70 from Bruker), see Figure A2 in Supplementary Information S3. The mean emissivity in the spectral range 5–25 µm is found to be in agreement with the fitted values. To calculate the mean emissivity we assumed the spectral emissivity to equal the measured spectral absorptivity and weighted it with the blackbody spectrum at \({T}_{0}\) = 294 K. Utilizing a DrudeLorentz model for the glass permittivity (Supplementary Information S3) we checked that increasing the spectral range has no impact on the mean emissivity, consistent with the spectral distribution of blackbody radiation. (In principle, the top and side emissivities can be different due to different roughness.) Fitted \({R}_{c}\) values were found to range from 5 to 11 K/W, while sensor/heater loss conductance \({h}_{sen}\) was found to vary from 0.3 to 5.5 W/(m²K) (below the blackbody heat flux of 5.76 W/(m²K) at 294 K).
Next, the gap sample measurement is fit using only one parameter, the gap resistance \({R}_{gap}\). Fitted \({R}_{gap}\) values ranged from 35.2 K/W for the smallest gap to 605 K/W for the largest gap. Fitted curves together with the measured ones are shown exemplarily for a 315 nm and a 2.75 µm gap in Fig. 3. Fits and measurements agree very well.
Qualitatively, the transient behavior can be described as follows: In the first few seconds the sensor/heater heats up to few hundred millikelvin above the ambient environment. This increased temperature is necessary for the heat to bridge the contact resistance \({R}_{c}\) and begin to mainly flow into the substrate instead of increasing the sensor/heater temperature. Because the thermal mass of the sensor/heater, \(m{c}_{sen}\), is small the temperature increases quickly. The larger \({R}_{c}\) is, the larger this initial temperature increase of the sensor/heater needs to be such that almost all the input power flows into the substrate. Note that as \({R}_{c}\ll 1/({h}_{sen}{A}_{sen})\) sensor/heater losses are irrelevant for these dynamics.
After this initial heating has occurred, the heat front begins moving from the bottom to the top of the substrate. This middle time span captures the bulk thermal properties of the sample. Separation between the two measurements begins as soon as the heat front has reached the top of the substrate. With the thermal properties of the glasses depicted in Supplementary Information S5, we calculated the time to reach the substrate top to be around 10 s. However, we want to emphasize that the separation is a slow and gradual process and thus takes another few tens of seconds until it is clearly visible. For reference sample measurements and gap sample measurements employing large gaps, in which case the upper disk practically keeps its initial temperature, the remaining dynamic is then governed by the sensor/heater and substrate heating up together while losing heat at the sensor/heater, the disk sides and the top/gap. The large thermal mass of the disks makes this dynamic significantly slower. Any changes to the top emissivity or gap conductance alter the shape of this portion of the transient. For smaller gaps, the NFRHT is large enough to allow the superstrate disk to heat up significantly, producing dramatic alterations to the shape of the transient curve.
In principle, all the variables can be obtained directly from the gap measurement without the need for a reference. Following the above description, unique identification is possible as each parameter influence the transient in a different way. E.g. \({R}_{c}\) is proportional to the initial steep temperature increase in the first few seconds, whereas \({R}_{gap}\) start to influence the transient only after some time, the time the two curves in Fig. 3 start to deviate. However, in our particular setup, the sensor/heater losses \({h}_{sen}\) and gap conductance \(1/{R}_{gap}\) have a similar effect on the transient; and while differentiation is theoretically possible, due to the delayed influence of the gap conductance vs. the nondelayed influence of the sensor/heater losses, it is not practical. An improved design with a better, e.g. active, thermal insulation may reduce \({h}_{sen}\) to negligibly small values and render the problem void. Similarly, sensor/heater losses \({h}_{sen}\) and side losses \({\varepsilon }_{side}\) have a combined effect, not distinguishable in practice. However, a differentiation is not needed to obtain the gap heat flux. Nevertheless, the twostep gapreference measurement procedure outlined above provides extra information without introducing new unknowns, and increases both the certainty and accuracy of the fitted results.
Note that the temperature transients in Fig. 3 have not yet reached a steady state. Theoretically, their exponential characteristic prevents the transients to ever reach steady state. However, due to environmental fluctuations, we can say the system is practically in steady state when the temperature is only a few percent away from its steadystate value. Using our 1D model we estimated for the gap setup the time till sensor/heater temperature becomes less than 5% below its steadystate value. The time ranges from 2200 s to 4100 s, depending on the concrete parameters. This coincides with settling times of 3060 min reported for nearfield measurements of centimeter sized samples^{40,43}. In any case, our measurement time of 640 s is more than three times shorter than the settling time. An even shorter measurement time can be envisaged as the deviation between gap and reference measurements is visible already after 200 s.
Data availability
The authors declare that the data supporting the findings of this study are available within the article and its Supplementary Information file. The raw measurement data are available from the corresponding author on reasonable request.
Results
Figure 4 shows the heat transfer coefficient (HTC) – the thermal power flow across the gap per unit cross sectional area per unit temperature difference – normalized to the blackbody HTC \({h}_{bb}\) = 5.76 W/(m²·K) (at 294 K) for different gap sizes. Each of the points corresponds to one measurement. The error margin in the horizontal axis corresponds to the error in the determination of the gap size (see Supplementary Material S6). The relative gap size error increases for the smaller gaps. The vertical error margins in Fig. 4 represent our measurement inaccuracy and combine the effects from fitting procedure and parameter changes between gap and reference measurements. The uncertainty for each measurement is the quadrature of an up to 8% fitting uncertainty, and a 10% variation accounting for possible changes in the sensor/heater losses between gap and reference measurement. The individual contributions are not summed up but the square root of the sum of their squares is taken (root sum square). This leads to an estimated inaccuracy of up to ±13%.
To confirm the reproducibility of the measured results we repeated measurements for the fused silica optical flats with 1.3 µm gap. In addition, the number of deposited microspheres (spacers) was systematically decreased in five measurements to determine the influence of the heat conduction through the microspheres on the apparent radiative HTC. Also, the measurement with the smallest number of particles was repeated four times to check the reproducibility. For additional details see Supplementary Information S2. These series of measurements exhibited no clear trend of the heat flux and a standard deviation of 7.5% which is within the measurement accuracy.
For the 150 nm gap the resistance between the substrate and superstrate becomes comparable to the disks’ inner resistance. Consequently, the influence of this variable on the transient is weaker than for larger gaps and the variation accounting for possible changes in sensor/heater losses becomes 20% instead of 10%. Additional details are provided in Supplementary Information S7.
The theoretical areas are calculated using the wellknown integral expression for the nearfield heat flux between two half spaces first established by Polder and van Hove.^{3,4,5}. As the optical properties of our samples are known only within a given margin of uncertainty the theoretical HTC is represented as an area, rather than single line. The optical properties used are examined in Supplementary Information S3, and further details of the calculation presented in Supplementary Information S4.
The measured HTCs are observed to be in good agreement with the theoretically predicted range of NFRHT. With decreasing gap size the HCT predictably increases due to the increasing contribution of evanescent modes, consistent with Rytovian electrodynamics^{2,3,4,7}. Besides, confirming our dynamic measurement approach, the measurements themselves are notable. The recorded nearfield heat flux ~16 times above the blackbody for the 150 nm gap is presently the largest recorded radiative enhancement for centimeter sized samples at ambient temperatures. At the smallest gap size the surface modes^{7,8}, supported by our fused silica samples, create a significantly larger enhancement of the heat flux as compared to purely dielectric samples^{47}. We also note that the creation of a gap as small as 150 nm over macroscopic cross sections has previously been reported in only one other experiment^{47}, where only an 8.4 heat flux enhancement over blackbody was demonstrated.
For larger gaps a small systematic overestimation of the HTC is observed. We attribute this ≈20% offset to the solid conduction through the supporting microspheres (Supplementary Information S2). Their contribution is reduced at smaller gap sizes as the solid conductance approaches a constant value and the radiative conductance approaches square of inverse gap size dependency. However, it should be noted that the HTC is unequivocally dominated by radiation for all gap sizes (Supplementary Information S2).
Discussion
The additional information contained in any dynamic or transient approach is both a strength and weakness compared to steadystate measurement techniques. Fundamentally, the measurement is not direct, and the desired parameters are only obtained by iteratively solving an inverse problem. Even for a relatively simple system, like the one we have considered, this introduces the need to carefully consider issues like numerical accuracy, initial values for system parameters, and generally increases the complexity of data analysis.
In return, the strict conditions that are required for a stationary measurement are relaxed. Steadystate measurements require at least three sensors: one sensor for measuring the temperature on each side of the gap, and additional flux sensor for measuring either the heating or cooling power. (Note that the flux sensor may be incorporated as part of the temperature sensor as it is in the TPS method). Crucially, there must be only one undetermined thermal resistance between these sensors. If it is not possible to isolate the NFRHT in this way, then prior to measurement all other heat conduction pathways must be properly modeled before any measurements can be made. Comparatively, in a transient approach the influence of a resistance varies relative to its position from the sensor/heater. The further away from the sensor/heater it is, the later its influence starts. This segregation of effects based on their temporal influence range has three primary benefits. First, it allows the gap resistance to be distinguished from other (parasitic) resistances in the system from collected data (a posteriori). Second, it allows the sensor/heater to be moved away from gap, separating and protecting the gap which is probed from (influences of) the measuring setup. Third, it allows for the simultaneous determination of solid state thermal characteristics that must be assumed in steadystate measurements, and would allow for more than one gap resistance to be determined in a multi gap setup^{56}. As mentioned in the introduction, there may also be significant differences in the time needed to perform an individual measurement. For a dynamic measurement the characteristic duration is determined by the distance that must be traveled by the thermal wave front before the influence of the unknown parameter begins to affect the shape of the transient.
In some experiments, to isolate the NFRHT from other parasitic heat fluxes, the gap size has been modulated with a constant frequency and only the heat flux varying with the same frequency has been analyzed^{14,19,20,24,36,46}. Further, analogues of 3ω measuring method have also been pursued^{25,36,46}. These are certainly counterparts to the reported technique, but they are not dynamic in sense that measurement remains steadystate. At present, no analogue of the dynamic laser flash, transient line, or plane source methods used routinely in measuring solid thermal properties exists for NFRHT measurements.
For academic settings, particularly if all the other thermal characteristics of a given sample are known, these advantages are clearly minimized. Generally, samples are very small and can be carefully designed with multiple micro/nanofabrication steps. Nevertheless, as NFRHT technologies develop it is highly likely that this will not remain the case. Under even slightly different circumstances, the comparative ability of a dynamic approach to quickly and reliably characterize a variety of samples and reduce design complexity could become critically important. (These considerations extend to any transient technique, and the method we have presented here could, for example, be used in a laser flash system.) It is also worth noting that dynamic measurements are a vital step towards analyzing and implementing systems which make use of dynamic effects, which, by definition, cannot be investigated by steadystate measurements.
Summary
In summary we have developed a new, dynamic nearfield radiative heat transfer measuring method, the first of its kind for this application. Using gap and reference sample types employing two different glass materials and gaps varying from 7 μm to 150 nm we have experimentally confirmed the ability of the approach to accurately measure nearfield thermal radiative heat transfer. For the 150 nm gap the measured heat flux is as large as ~16 times above the blackbody. Advantages of this method include simple and precise referencing, the lack of required micro/nano fabrication, and the ability to temporally resolve the influence of various thermal parameters; which helps to distinguish the gap conduction from other effects like interface resistances. The method can also easily be modified and extended. Our results bring to light so far neglected transient measurement techniques, and open the door for the investigation of dynamic radiative effects.
References
 1.
Planck, M. The theory of heat radiation (Courier Corporation, 1959).
 2.
Basu, S., Zhang, Z. M. & Fu, C. J. Review of nearfield thermal radiation and its application to energy conversion. Int. J. Energy Res. 33, 1203–1232 (2009).
 3.
Park, K. & Zhang, Z. Fundamentals and applications of nearfield radiative energy transfer. Front. Heat Mass Transfer 4, 013001 (2013).
 4.
Polder, D. & van Hove, M. Theory of Radiative Heat Transfer between Closely Spaced Bodies. Phys. Rev. B 4, 3303–3314 (1971).
 5.
Biehs, S.A., Rousseau, E. & Greffet, J.J. Mesoscopic Description of Radiative Heat Transfer at the Nanoscale. Phys. Rev. Lett. 105, 234301 (2010).
 6.
Otey, C. R., Zhu, L., Sandhu, S. & Fan, S. Fluctuational electrodynamics calculations of nearfield heat transfer in nonplanar geometries: A brief overview. J. Quant. Spect. Rad. Transf. 132, 3–11 (2014).
 7.
Joulain, K., Mulet, J.P., Marquier, F., Carminati, R. & Greffet, J.J. Surface electromagnetic waves thermally excited: Radiative heat transfer, coherence properties and Casimir forces revisited in the near field. Surf. Sci. Rep. 57, 59–112 (2005).
 8.
Basu, S. & Zhang, Z. M. Ultrasmall penetration depth in nanoscale thermal radiation. Appl. Phys. Lett. 95, 133104 (2009).
 9.
Guo, Y., Cortes, C. L., Molesky, S. & Jacob, Z. Broadband superPlanckian thermal emission from hyperbolic metamaterials. Appl. Phys. Lett. 101, 131106 (2012).
 10.
Biehs, S.A., Tschikin, M. & BenAbdallah, P. Hyperbolic Metamaterials as an Analog of a Blackbody in the Near Field. Phys. Rev. Lett. 109, 104301 (2012).
 11.
Nefedov, I. S. & Simovski, C. R. Giant radiation heat transfer through micron gaps. Phys. Rev. B 84, 195459 (2011).
 12.
Simovski, C., Maslovski, S., Nefedov, I. & Tretyakov, S. Optimization of radiative heat transfer in hyperbolic metamaterials for thermophotovoltaic applications. Opt. Express 21, 14988–15013 (2013).
 13.
Lang, S. et al. Large penetration depth of nearfield heat flux in hyperbolic media. Appl. Phys. Lett. 104, 121903 (2014).
 14.
DiMatteo, R. S. et al. Enhanced photogeneration of carriers in a semiconductor via coupling across a nonisothermal nanoscale vacuum gap. Appl. Phys. Lett. 79, 1894 (2001).
 15.
Narayanaswamy, A. & Chen, G. Surface modes for near field thermophotovoltaics. Appl. Phys. Lett. 82, 3544 (2003).
 16.
Laroche, M., Carminati, R. & Greffet, J.J. Nearfield thermophotovoltaic energy conversion. J. Appl. Phys. 100, 63704 (2006).
 17.
Park, K., Basu, S., King, W. P. & Zhang, Z. M. Performance analysis of nearfield thermophotovoltaic devices considering absorption distribution. J. Quant. Spect. Rad. Transf. 109, 305–316 (2008).
 18.
Huth, F., Schnell, M., Wittborn, J., Ocelic, N. & Hillenbrand, R. Infraredspectroscopic nanoimaging with a thermal source. Nat. Mater. 10, 352–356 (2011).
 19.
De Wilde, Y. et al. Thermal radiation scanning tunnelling microscopy. Nature 444, 740–743 (2006).
 20.
Babuty, A., Joulain, K., Chapuis, P.O., Greffet, J.J. & De Wilde, Y. Blackbody Spectrum Revisited in the Near Field. Phys. Rev. Lett. 110, 146103 (2013).
 21.
Kittel, A. et al. NearField Heat Transfer in a Scanning Thermal Microscope. Phys. Rev. Lett. 95, 224301 (2005).
 22.
Kittel, A. et al. Nearfield thermal imaging of nanostructured surfaces. Appl. Phys. Lett. 93, 193109 (2008).
 23.
Worbes, L., Hellmann, D. & Kittel, A. Enhanced NearField Heat Flow of a Monolayer Dielectric Island. Phys. Rev. Lett. 110, 134302 (2013).
 24.
Jones, A. C. & Raschke, M. B. Thermal Infrared NearField Spectroscopy. Nano Lett. 12, 1475–1481 (2012).
 25.
Kim, K. et al. Radiative heat transfer in the extreme near field. Nature 528, 387–391 (2015).
 26.
O’Callahan, B. T. & Raschke, M. B. Laser heating of scanning probe tips for thermal nearfield spectroscopy and imaging. APL Photonics 2, 021301 (2016).
 27.
Kloppstech, K. et al. Giant heat transfer in the crossover regime between conduction and radiation. Nat. Commun. 8, 14475 (2017).
 28.
Rousseau, E. et al. Radiative heat transfer at the nanoscale. Nat. Photon. 3, 514–517 (2009).
 29.
Narayanaswamy, A., Shen, S. & Chen, G. Nearfield radiative heat transfer between a sphere and a substrate. Phys. Rev. B 78, 115303 (2008).
 30.
Shen, S., Narayanaswamy, A. & Chen, G. Surface Phonon Polaritons Mediated Energy Transfer between Nanoscale Gaps. Nano Lett. 9, 2909–2913 (2009).
 31.
Shen, S., Mavrokefalos, A., Sambegoro, P. & Chen, G. Nanoscale thermal radiation between two gold surfaces. Appl. Phys. Lett. 100, 233114 (2012).
 32.
Guha, B., Otey, C., Poitras, C. B., Fan, S. & Lipson, M. NearField Radiative Cooling of Nanostructures. Nano Lett. 12, 4546–4550 (2012).
 33.
van Zwol, P. J., Ranno, L. & Chevrier, J. Emissivity measurements with an atomic force microscope. J. Appl. Phys. 111, 063110 (2012).
 34.
van Zwol, P. J., Ranno, L. & Chevrier, J. Tuning Near Field Radiative Heat Flux through Surface Excitations with a Metal Insulator Transition. Phys. Rev. Lett. 108, 234301 (2012).
 35.
Shi, J., Liu, B., Li, P., Yen Ng, L. & Shen, S. NearField Energy Extraction with Hyperbolic Metamaterials. Nano Lett. 15, 1217–1221 (2015).
 36.
Song, B. et al. Enhancement of nearfield radiative heat transfer using polar dielectric thin films. Nat. Nanotechnol. 10, 253–258 (2015).
 37.
Hargreaves, C. M. Anomalous radiative transfer between closelyspaced bodies. Phys. Lett. 30A, 491–492 (1969).
 38.
Domoto, G. A., Boehm, R. F. & Tien, C. L. Experimental Investigation of Radiative Transfer Between Metallic Surfaces at Cryogenic Temperatures. J. Heat Transfer 92, 412–416 (1970).
 39.
Hu, L., Narayanaswamy, A., Chen, X. & Chen, G. Nearfield thermal radiation between two closely spaced glass plates exceeding Planck’s blackbody radiation law. Appl. Phys. Lett. 92, 133106 (2008).
 40.
Ottens, R. S. et al. NearField Radiative Heat Transfer between Macroscopic Planar Surfaces. Phys. Rev. Lett. 107, 014301 (2011).
 41.
Kralik, T. et al. Strong NearField Enhancement of Radiative Heat Transfer between Metallic Surfaces. Phys. Rev. Lett. 109, 224302 (2012).
 42.
Feng, C., Tang, Z., Yu, J. & Sun, C. A MEMS Device Capable of Measuring NearField Thermal Radiation between Membranes. Sensors 13, 1998–2010 (2013).
 43.
Ijiro, T. & Yamada, N. Nearfield radiative heat transfer between two parallel SiO_{2} plates with and without microcavities. Appl. Phys. Lett. 106, 023103 (2015).
 44.
Ito, K., Miura, A., Iizuka, H. & Toshiyoshi, H. Parallelplate submicron gap formed by micromachined lowdensity pillars for nearfield radiative heat transfer. Appl. Phys. Lett. 106, 083504 (2015).
 45.
Lim, M., Lee, S. S. & Lee, B. J. Nearfield thermal radiation between doped silicon plates at nanoscale gaps. Phys. Rev. B 91, 195136 (2015).
 46.
Song, B. et al. Radiative heat conductances between dielectric and metallic parallel plates with nanoscale gaps. Nat. Nanotechnol. 11, 509–514 (2016).
 47.
Bernardi, M. P., Milovich, D. & Francoeur, M. Radiative heat transfer exceeding the blackbody limit between macroscale planar surfaces separated by a nanosize vacuum gap. Nat. Commun. 7, 12900 (2016).
 48.
StGelais, R., Zhu, L., Fan, S. & Lipson, M. Nearfield radiative heat transfer between parallel structures in the deep subwavelength regime. Nat. Nanotechnol. 11, 515–519 (2016).
 49.
StGelais, R., Guha, B., Zhu, L., Fan, S. & Lipson, M. Demonstration of Strong NearField Radiative Heat Transfer between Integrated Nanostructures. Nano Lett. 14, 6971–6975 (2014).
 50.
Gustafsson, S. E. Transient plane source techniques for thermal conductivity and thermal diffusivity measurements of solid materials. Rev. Sci. Instrum. 62, 797 (1991).
 51.
Gustavsson, M., Karawacki, E. & Gustafsson, S. E. Thermal conductivity, thermal diffusivity, and specific heat of thin samples from transient measurements with hot disk sensors. Rev. Sci. Instrum. 65, 3856 (1994).
 52.
“Kapton General Specifications” from DuPont, downloadable at www.dupont.com (2017).
 53.
Benford, D. J., Powers, T. J. & Moseley, S. H. Thermal conductivity of Kapton tape. Cryogenics 39, 93–95 (1999).
 54.
Crank, J. & Nicolson, P. A practical method for numerical evaluation of solutions of partial differential equations of the heatconduction type. Math. Proc. Cambridge Philos. Soc 43, 50–67 (1947).
 55.
Dawson, C. N., Du, Q. & Dupont, T. F. A finite difference domain decomposition algorithm for numerical solution of the heat equation. Math. Comp. 57, 63–71 (1991).
 56.
BenAbdallah, P. & Biehs, S.A. NearField Thermal Transistor. Phys. Rev. Lett. 112, 044301 (2014).
Acknowledgements
The authors from Hamburg University of Technology gratefully acknowledge financial support from the German Research Foundation (DFG) via SFB 986 “M³”, project C1. S. M. and Z. J. gratefully acknowledge support from the Natural Sciences and Engineering Research Council of Canada (NSERC), Alberta Innovates Technology Futures (AITF), and the HelmholtzAlberta Initiative. This publication was supported by the German Research Foundation (DFG) and the Hamburg University of Technology (TUHH) in the funding programme Open Access Publishing.
Author information
Affiliations
Contributions
A.Y.P., S.M. and S.L. developed the measuring technique. G.S., S.M., P.U.K. and T.J. performed the measurements. S.L., G.S., S.M. and P.U.K contributed to the analyses of experimental data. A.Y.P., Z.J. and M.E. supervised the project. All authors discussed the results of the manuscript and provided comments for its finalization.
Corresponding author
Ethics declarations
Competing Interests
The authors declare that they have no competing interests.
Additional information
Publisher's note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Electronic supplementary material
Rights and permissions
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
About this article
Cite this article
Lang, S., Sharma, G., Molesky, S. et al. Dynamic measurement of nearfield radiative heat transfer. Sci Rep 7, 13916 (2017). https://doi.org/10.1038/s4159801714242x
Received:
Accepted:
Published:
Further reading

NearField Radiative Heat Transfer between Dissimilar Materials Mediated by Coupled Surface Phonon and PlasmonPolaritons
ACS Photonics (2020)

Strong suppression of nearfield radiative heat transfer by superconductivity in NbN
Physical Review B (2019)

NearField Radiative Heat Transfer around the Percolation Threshold in Al Oxide Layers
The Journal of Physical Chemistry C (2019)

Material scaling and frequencyselective enhancement of nearfield radiative heat transfer for lossy metals in two dimensions via inverse design
Physical Review B (2019)

A nearfield radiative heat transfer device
Nature Nanotechnology (2019)
Comments
By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.