Overcoming the Negative Energy Density Requirements in the Alcubierre Warp Field Equations with a Complex Shaping Function
Chance M. Glenn
Open licence · full text · Creative Commons Attribution License (CC BY)
In one page
Chance M. Glenn of Alabama A&M University takes the one number that has haunted the Alcubierre warp metric since 1994 — the required energy density comes out negative — and asks whether the sign is forced by the mathematics or by a choice inside it. Alcubierre's energy density depends on the square of the derivative of the shaping function, the profile that describes how spacetime is squeezed ahead of a craft and stretched behind it. Glenn lets that shaping function be complex, and shows that when the imaginary part is larger than the real part the square turns negative and the required energy density turns positive — ordinary, non-exotic energy. He then proposes hardware for it: a cylindrical resonant cavity, a warp core, filled with a lossy dielectric whose permittivity is more imaginary than real, driven at 2.4 GHz, with a laser threaded down the middle to look for a deflection. He built it, and reports honestly that the bench energy density is orders of magnitude short.
Why it matters hereChapter 4's central question is whether metric engineering needs exotic matter or only clever geometry, and this paper argues the exotic requirement is an artefact of assuming a real-valued shaping function. It also does what chapter 13 asks of a proposal: it names the material, the frequency, the cavity dimensions and the measurement, so the next person can build a better version rather than argue about it.
What it claims
01Solving Alcubierre's energy density expression for the derivative of the shaping function shows that this derivative must be complex if the required energy density is to be positive, because the energy density is proportional to the square of that derivative.Section 'Introducing a Complex Shaping Function', Equations 4 and 5
Published and peer-reviewed02Writing the shaping function as a real coefficient plus an imaginary coefficient times the original profile, the square of its derivative picks up a factor equal to the squared real part minus the squared imaginary part; if the imaginary part is the larger, that factor is negative and the required energy density distribution becomes positive and non-exotic.Equations 6 to 9; Figure 3, the map of total required energy over the complex plane
Published and peer-reviewed03With the real coefficient at 0.2 and the imaginary coefficient at 0.6, the Alcubierre top-hat profile keeps the Yorke time structure that matters — spacetime compressed ahead of the craft, expanded behind, and a region of undisturbed spacetime where the passengers sit — while the energy density distribution comes out positive.Figure 4; simulations for quarter-cosine, cosine-squared and sinc profiles at an apparent velocity of ten times light speed with a one-metre bubble radius, Figures 5 to 7
Published and peer-reviewed04The proposed physical realisation is a cylindrical resonant cavity — a warp core — filled with a lossy dielectric of complex relative permittivity 12.21 plus 14.52i at 2.4 GHz and 20 degrees Celsius, driven in the TM010 transverse magnetic mode, in which the electric flux density inside the cavity plays the part of the shaping function; the cavity radius is 8.9 mm with a 1.5 mm pass-through hole for a laser beam.Section 'Realization', Equations 10 to 12, Figures 8 and 9; Table 1, Rf Cavity Experiment Parameters
Designed, not yet built05In the bench experiment, lasers at 410, 532 and 650 nanometres passed through the energised cavity produced no appreciable fluctuation in the photodetector output; the back-of-the-envelope energy density reached in the cavity at 100 mW of rf input is far short of the level the metric requires.Sections 'Experiment' and 'Results', Equations 13 to 15; Table 1
What to watch06The named routes to a stronger test are pulsed power, to establish a higher differential energy with respect to the radius; concentrating a higher input energy over a smaller region; and metamaterials inside the rf chamber to build the complex structure.Section 'Results', final paragraph; Summary
What to watch
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Abstract
In this paper we show that the use of a resonant cavity filled with a lossy dielectric can overcome the negative energy density requirement in Alcubierre’s warp field equations. By using an imaginary part equal to or greater than the real part in the shaping function we generate a positive, non-exotic energy density requirement to generate and sustain the warp bubble necessary to transport a craft through space. We show simulation results for various shaping functions, the resulting Yorke time deformation, and the energy density over the warp bubble required. We discuss potential realizations of a device which generates such a field using electromagnetic and rf theory. Finally, we propose and show results of a simple experiment that uses these principles.
Keywords: Alcubierre, Warp Bubble, Spacetime, Yorke Time, Space Travel, Relativity, Electromagnetics, Resonance, Dielectric.
Key passages
The following passages are quoted from the article under its Creative Commons Attribution License, with attribution to Chance M. Glenn, "Overcoming the Negative Energy Density Requirements in the Alcubierre Warp Field Equations with a Complex Shaping Function", Journal of Material Sciences and Engineering Technology, volume 4, issue 1, pages 1 to 7, 2026. The figures, the typeset equations and the reference list are not reproduced here; the complete article is free to read at the DOI.
The shaping function, and why it is the load-bearing choice
"In Alcubierre’s seminal paper he describes the possibility of moving a ship through by compressing spacetime in front of the craft and expanding it behind the craft, thus producing an apparent velocity in a given direction. This warping of spacetime can produce apparent velocities that well exceed the speed of light yet does not violate Einstein’s speed of light limit."
"The shaping function is an expression that describes the characteristics of the warp field that needs to be created to provide movement in the desired direction and is a function of the radius from the center of the ship… What is desirable about the specific shaping function used is that it provides no space time distortion within a region where the ship can reside. Therefore, the passengers suffer no effects of time dilation or length contraction/expansion within that region."
"There are no restrictions on the form of the shaping function, other than it would be beneficial to provide a region of unaffected spacetime wherein passengers can reside. As we will discuss in the next section, the required energy density is impacted by the shaping function."
Energy density
"The expression that is derived by Alcubierre for the required energy density is developed by calculating the Einstein tensor… It provides negative values for the energy density which violates conditions for weak, dominant, and strong energy conditions as set forth by Hawking. This suggests that the only way to form a warp bubble having any realizable shaping function is through the application of negative, or exotic, energy. While there has been much work engaged in reducing the resulting magnitude of this energy from the equivalent of mass contained within the entire known universe to that of the mass of a small space vehicle, the solution is still a negative value."
"The energy density expression is proportional to the square of the derivative of the shaping function with respect to the radius. For the shaping function described in equation (2) the energy density is large and negative over the region containing the warp field… The total energy is found by integrating over the whole space."
"In the next section we’ll describe how we can create a shaping function that still maintains a region unaffected by Yorke time expansion and contraction yet allows the solution to the energy density equation to yield positive values."
Introducing a complex shaping function
"If we solve equation (4) for the derivative of the shaping function… which suggests that the derivative of the shaping function with respect to the radius must be complex if we are to have a positive energy density requirement."
"Therefore if the magnitude of the imaginary coefficient is greater than the magnitude of the real coefficient then the square of the derivative of the shaping function with respect to the radius is negative, which allows the required energy density distribution to be positive, and perhaps even be in more of a manageable magnitude."
"Now if we select the values 0.2 for the real coefficient and 0.6 for the imaginary coefficient then we see the energy density distribution shown in Figure 4, which also provides the desired Yorke time structure as before."
Simulation results
"The top hat shaping function that been proposed is ideal for creating a region of normal spacetime within the warp bubble. As White pointed out the size and thickness of the warp bubble has a significant impact on the energy density requirement. In the following discussion we will look at three additional shaping functions and the energy required as a result."
"In our simulation we will look at (1) a quarter cosine function whose peak is at the center of the ship position and is zero at the bubble radius. We will look at (2) a cosine squared function that is zero at the bubble radius, and (3) a sinx/x function that is damped as it approaches the bubble radius. For each simulation the apparent velocity is ten times the speed of light, the radius of the warp bubble is 1 meter, and the ‘ship’ sits in the center of the warp field."
Realization
"Einstein postulated that the gravitational pull between two bodies was due to the bending of space time that occurs due to the mass of the objects. The Alcubierre metric was formulated from Einstein’s gravitational field equation formalism. Furthermore, there exists a relationship between gravitational field equations and Maxwell’s equations, which describe electromagnetic interactions. Electromagnetism can be formulated mathematically in Minkowski space. This suggests that electromagnetic fields have the potential to affect space time. The converse is clearly true as we are aware that strong gravitational fields bend light, which can be characterized as an electromagnetic wave."
"Our strategy is to construct a ‘warp core’ from a resonant cavity filled with a dielectric material with complex permittivity."
"Inside of the cavity, the shaping function is essentially the electric flux density. Under a transverse magnetic mode, particularly TM010, the field strength is maximum at the center of the cavity. We have identified a liquid material that has the complex permittivity of 12.21 plus 14.52i at a frequency of around 2.4 GHz and a temperature of 20 degrees C. As we showed in the previous section, if the imaginary part of the shaping function is greater than the real part, then the energy density distribution required to distort spacetime (Yorke time) in the manner shown is positive."
"The diameter of the cylinder is calculated as a half wavelength in the material to be used… In order to establish a TM010 mode the radius of the cavity will be 8.9 mm… Our goal is to demonstrate that a region of warped spacetime is created at the center of the cavity. The cavity is made such that there is a hole down the center which will allow a laser beam to pass through it unimpeded. If there is a perturbation of spacetime anywhere within this region, the laser beam will be slightly deflected."
"Under these conditions we expect the energy density to be that which is shown in Figure 10(a). It is positive and highest on the outer edges of the radius. The Yorke time response in Figure 10(b) shows that in the region ahead of the ‘ship’ spacetime is compressed and it is expanded in the region behind. There is only a negligible region where no spacetime compression or expansion occurs. The experimental process in this situation is such that we hope to observe some level of spacetime effect. Should this be effective then work can be done on the geometry or in the distribution of the dielectric material to produce a more useful shaping function."
Experiment and setup
"Our goal is to determine if it is possible to initiate and detect any warping of space time by establishing an energy distribution within a confined space having a profile like what Alcubierre and White postulated. Any fluctuation, or distortion in space time would affect the trajectory of a beam of light that passes through that region. We set up a basic experiment to detect any deviation in the intensity or phase of a beam of light that passes through a region of a cavity having a rf field established in the manner simulated above."
"A 650 nm laser beam is passed through the rf cavity through the pass-through hole. It is captured by an optical sensor whose voltage is measured by an oscilloscope. The rf cavity is fed by a continuous 2.4 GHz source at approximately 100 mW of power. Any fluctuations in voltage output to the scope will indicate that the laser beam has been affected by alteration in spacetime near it."
The experiment parameters given in Table 1 are: cylindrical cavity diameter 17.8 mm; pass-through hole diameter 1.5 mm; rf source power 100 mW; rf source frequency 2.4 GHz; laser wavelengths 410, 532 and 650 nm; real impedance in cavity 78 ohms.
Results
"After several attempts with three types of lasers, we observed no appreciable fluctuations in the voltage output on the oscilloscope when we introduced the rf into the dielectric filled cavity. This is not unexpected given that the energy densities required are several orders of magnitude higher than what we were able to produce with this bench top experiment."
"…which is far short of the required energy density levels to distort spacetime. As the goal here is to initiate the warping of spacetime in a local region it would be advantageous to determine a minimum required energy density to do so. Obousey proposes a minimal energy density requirement based on the Hubble constant but like White, suggests that this extremely high value can be reduced by thinner walls at the edge of the warp bubble. We also recommend pulsed power in order to establish a higher differential energy with respect to the radius. In addition, if higher input energy is concentrated over a smaller region, then the energy density is higher."
Summary
"We have established mathematically that there exists the potential to realize a positive required energy density in order to warp space time. By using a complex shaping function where the imaginary part is greater than the real part, the solution to the expression for the required energy density is positive. This ultimately makes it feasible to selectively bend spacetime for the purposes of propelling a craft."
"We have devised an experiment that utilizes a material having the properties of possessing a greater imaginary component to the dielectric constant than real component. This material, introduced into a resonant cavity, sets up the conditions to realize a shaping function in the form as is utilized in the Alcubierre’s metric. While we were not able to detect a distortion to spacetime we have established a potential structure from which to build better experiments."
"Additional considerations are to utilize metamaterials within a rf chamber or cavity for the establishment of a complex structure. By setting the stage for a positive energy density to warp space time we move much closer to realizing this extraordinary technological capability."
(Key passages only, reproduced under CC BY with attribution; the complete article, with all twelve figures and the full equations, is free to read at the DOI. On this site, Alcubierre’s original 1994 paper is at /library/stm-fc5383ec73, Harold White’s reworking of the energy requirement — the thin-shell argument Glenn cites — is at /library/stm-20c8a9090c, the anisotropic-matter modification of the metric and how a warp field might be detected is at /library/stm-634af34cf8, the supersymmetry-breaking Casimir route to the same goal is at /library/stm-7dfda7640a, the positive-energy warp solutions from hidden geometric structures are at /library/stm-3f01ca8468, and the causality question the metric raises is at /library/stm-f4d19d87a4.)
The way in
https://doi.org/10.61440/jmset.2026.v4.104Published as a Research Article in the Journal of Material Sciences and Engineering Technology, volume 4, issue 1, pages 1 to 7, received 31 January 2026, accepted 6 February 2026, published 13 February 2026, by OASK Publishers, ISSN 2977-0041. The licence is confirmed from the statement printed on the last page of the article itself: ‘Copyright: © 2026 Chance M Glenn. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.’ The abstract and the key passages below are reproduced under that licence with attribution to the author; the figures, the equations as typeset and the reference list are not reproduced, and the complete article is free to read at the DOI. The author is Chance M. Glenn of the College of Engineering, Technology and Physical Sciences, Alabama A&M University, Normal, USA; the library’s fetched record carried an empty first author entry, which is corrected here.
How to cite it
Chance M. Glenn (2026) Overcoming the Negative Energy Density Requirements in the Alcubierre Warp Field Equations with a Complex Shaping Function. doi:10.61440/jmset.2026.v4.104
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