Recognition: 2 theorem links
· Lean TheoremNumerical Investigations of Stable Dynamics in the Presence of Ghosts
Pith reviewed 2026-05-13 07:58 UTC · model grok-4.3
The pith
Ghost-normal scalar field systems can maintain dynamically bounded evolution for extended times when initial data favors ultraviolet modes and small amplitudes.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Ghost-normal systems can exhibit long-lived, dynamically bounded evolution over extended time intervals, with stability strongly controlled by spectral content and amplitude. Ultraviolet-dominated and small-amplitude configurations remain stable significantly longer than infrared-dominated or large-amplitude data, indicating that instability is mediated by nonlinear spectral energy transfer rather than instantaneous runaway. Nonlinear self-interactions play a dual role: while they can accelerate energy exchange between sectors, certain potentials generate transient metastable regimes that partially suppress ghost-induced growth.
What carries the argument
Spacetime finite-element discretization of two coupled scalar fields carrying opposite-sign kinetic terms, used to evolve broad classes of initial data in one and two spatial dimensions.
If this is right
- Instability develops through gradual nonlinear transfer of energy between the normal and ghost sectors rather than linear exponential growth.
- Initial data dominated by high-frequency modes and small overall amplitude postpones the onset of instability.
- Potentials that admit oscillon-like structures can temporarily suppress ghost-induced growth and create metastable intervals.
- The overall dynamical outcome depends on the balance of dispersion, nonlinearity strength, and phase structure rather than the mere presence of a ghost.
Where Pith is reading between the lines
- If the discretization is faithful, classical field theories containing ghosts need not collapse on short timescales and may admit long-lived metastable configurations.
- The same numerical strategy could be used to test whether analogous metastability appears in higher dimensions or with gravitational coupling.
- Observing persistent oscillon-like objects in ghost models would connect these results to soliton stability questions in other nonlinear theories.
Load-bearing premise
The finite-element grid reproduces the continuous equations without adding artificial damping or dispersion that would hide genuine ghost-driven growth.
What would settle it
A sufficiently long simulation starting from ultraviolet-dominated small-amplitude data that eventually shows unbounded growth or loss of boundedness would falsify the reported stability hierarchy.
Figures
read the original abstract
We explore the nonlinear dynamics of classical field theories containing ghost degrees of freedom, focusing on two coupled scalar fields with opposite kinetic terms in (1+1) and (2+1) dimensional Minkowski spacetime. Using a spacetime finite element formulation, we perform a systematic numerical study across a broad class of initial data. We find that ghost-normal systems can exhibit long-lived, dynamically bounded evolution over extended time intervals, with stability strongly controlled by spectral content and amplitude. Ultraviolet-dominated and small-amplitude configurations remain stable significantly longer than infrared-dominated or large-amplitude data, indicating that instability is mediated by nonlinear spectral energy transfer rather than instantaneous runaway. Nonlinear self-interactions play a dual role: while they can accelerate energy exchange between sectors, certain potentials, including a lifted $\phi^6$ interaction supporting oscillon-like structures, generate transient metastable regimes that partially suppress ghost-induced growth. Our results demonstrate that the dynamical consequences of ghost modes in classical field theory depend sensitively on dispersion, nonlinearity, and phase structure, revealing a richer metastability landscape than commonly assumed.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports a numerical study of two coupled scalar fields with opposite-sign kinetic terms in (1+1) and (2+1)D Minkowski spacetime, using a spacetime finite element formulation. It claims that ghost-normal systems can exhibit long-lived bounded evolution over extended times, with stability strongly controlled by spectral content and amplitude: UV-dominated and small-amplitude initial data remain stable significantly longer than IR-dominated or large-amplitude data. Instability is attributed to nonlinear spectral energy transfer rather than instantaneous runaway, and certain potentials (including a lifted φ⁶ interaction) are shown to generate transient metastable regimes that partially suppress ghost-induced growth.
Significance. If the reported metastability accurately reflects the continuous dynamics, the work would demonstrate that ghost instabilities in classical field theories are not invariably immediate but can be delayed or modulated by dispersion relations, nonlinearity, and phase structure, revealing a richer metastability landscape. The systematic scan across initial-data classes is a positive feature. However, the numerical character of the study means its significance hinges on validation of the discretization.
major comments (1)
- [Abstract and numerical results] Abstract and numerical results: the central claim that UV-dominated configurations remain stable significantly longer depends on the spacetime finite element discretization faithfully reproducing the continuous dynamics. For systems with opposite-sign kinetic terms (non-hyperbolic), standard FEM stabilization can preferentially damp the high-frequency modes that mediate the nonlinear energy transfer described in the abstract. No mesh-convergence data, a-posteriori error estimates, or cross-validation against alternative discretizations are reported, so the observed metastability windows could be numerical artifacts rather than properties of the continuous theory.
minor comments (2)
- The abstract would benefit from a brief statement of the specific potentials and initial-data families used, to make the trends immediately quantifiable.
- Figure captions should explicitly state the simulation duration and mesh parameters for each panel to allow readers to assess the reported stability intervals.
Simulated Author's Rebuttal
We thank the referee for the careful reading and the constructive comment on numerical validation. We address the concern directly below and will strengthen the manuscript accordingly.
read point-by-point responses
-
Referee: [Abstract and numerical results] Abstract and numerical results: the central claim that UV-dominated configurations remain stable significantly longer depends on the spacetime finite element discretization faithfully reproducing the continuous dynamics. For systems with opposite-sign kinetic terms (non-hyperbolic), standard FEM stabilization can preferentially damp the high-frequency modes that mediate the nonlinear energy transfer described in the abstract. No mesh-convergence data, a-posteriori error estimates, or cross-validation against alternative discretizations are reported, so the observed metastability windows could be numerical artifacts rather than properties of the continuous theory.
Authors: We agree that explicit convergence diagnostics are required to substantiate the claims for a non-hyperbolic system. In the revised version we will add mesh-refinement studies in both (1+1)D and (2+1)D, demonstrating that the reported metastability lifetimes for UV-dominated, low-amplitude data converge under successive h-refinement. We will also include a-posteriori residual-based error estimates for representative runs. Our spacetime Galerkin formulation employs no artificial viscosity or high-mode damping; the weak form is consistent and the time integrator is implicit and energy-consistent. To address possible scheme dependence we will include a short cross-check against a second-order centered finite-difference discretization on a subset of initial data, confirming that the qualitative distinction between UV- and IR-dominated regimes persists. These additions will be placed in a new subsection of the numerical-methods section together with the existing spectral diagnostics. revision: yes
Circularity Check
No significant circularity in numerical study
full rationale
The paper performs direct numerical simulations of ghost-normal scalar field systems using a spacetime finite element discretization in (1+1) and (2+1) dimensions. All reported stability windows, spectral dependence, and metastability observations are generated by evolving initial data under the discretized equations of motion; no parameters are fitted to subsets of results and then invoked as predictions, no self-definitional equations appear, and no load-bearing uniqueness theorems or ansatzes are imported via self-citation. The central claims therefore rest on computational output rather than any derivation that reduces to its own inputs by construction.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The spacetime finite element method converges to the true solution of the continuous field equations as mesh size and time step approach zero.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel (J-cost uniqueness) unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
ghost-normal systems can exhibit long-lived, dynamically bounded evolution... stability strongly controlled by spectral content and amplitude... nonlinear self-interactions play a dual role
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Ostrogradsky theorem... degenerate higher-derivative theories... Galileons
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
We follow the dis- cretization scheme in [23, 24]
Space-Time Finite Element Method A space-time FEM uses continuous approximation functions in both space and time. We follow the dis- cretization scheme in [23, 24]. In this scheme, space and time are discretized together for the entire domain using a finite element space which does not discriminate be- tween space and time basis functions. In this way, we...
-
[2]
Setting Up The Weak Form Since the original system is second order in time, it is necessary for the weak formulation to introduce auxiliary variables such that our system can be reduced to one that is first order in time. Letu=∂ tϕandv=∂ tχ. From Eqns. 2 and 3, we 4 have ∂u ∂t − ∇2ϕ+m 2 ϕϕ+ ∂V ∂ϕ = 0,(16) ∂ϕ ∂t −u= 0,(17) ∂v ∂t − ∇2χ+m 2 χχ+γ ∂V ∂χ = 0,(1...
-
[3]
Nonlinear Solver: PETSc SNES In order to computationally handle the nonlinearity of the PDE system, we utilize PETSc’s SNES library. The library contains methods, like Newton’s method with line search, for solving nonlinear equations of the form F(U) = 0, whereFis the nonlinear differential operator, andUis the solution vector. The two main user-created c...
-
[4]
R k ←F(U k)(FormResidual()) 2.If∥R k∥ ≤rtol,stop (converged)
-
[5]
J k ← ∂F ∂U (Uk)(FormJacobian()) 4.SolveJ k δUk =−R k (KSP/PC linear solve, PETSc) 5.Choose stepα∈(0,1] (line search, PETSc)
-
[6]
U k+1 ←U k +α δU k (PETSc) TABLE I B. Initial Data In this section, we describe different initial conditions (IC) that are motivated by different physical implica- 5 tions. We first start with simple plane wave and Gaussian packet IC which are similarly explored in [21]. Then, we expand the discussion and explore more interesting sce- narios
-
[7]
where cϕ =± s k2 ϕ +m 2 ϕ k2 ϕ , cχ =± s k2χ +m 2χ k2χ
Plane waves The plane wave initial conditions are given by ϕ0(x) =A ϕ sin kϕ(x−x ϕ) , ˙ϕ0(x) =−c ϕ kϕ Aϕ cos kϕ(x−x ϕ) , χ0(x) =A χ sin kχ(x−x χ) , ˙χ0(x) =−c χ kχ Aχ cos kχ(x−x χ) . where cϕ =± s k2 ϕ +m 2 ϕ k2 ϕ , cχ =± s k2χ +m 2χ k2χ . (21) We fixx ϕ = 0,x χ =L/3,A ϕ =A χ =A,k ϕ =k χ/2 = k, and choose the two plane waves to move in opposite directions...
-
[8]
Gaussian packets The Gaussian wave packet initial data are defined by ϕ0(x) =A ϕ exp −(x−x ϕ)2 2ℓ2 ϕ ! , ˙ϕ0(x) =A ϕ cϕ(x−x ϕ) ℓ2 ϕ exp −(x−x ϕ)2 2ℓ2 ϕ ! , χ0(x) =A χ exp −(x−x χ)2 2ℓ2χ , ˙χ0(x) =A χ cχ(x−x χ) ℓ2χ exp −(x−x χ)2 2ℓ2χ , wherec ϕ andc χ are defined oppositely (1 and -1) so that the waves travel in opposite directions or defined equivalently ...
-
[9]
Colored-noise spectra (IR/UV-tilted) Choose integersn 1 ≤n≤n 2, phasesθ n ∈[0,2π), and a spectral tiltn s ∈R. Define ϕ(x,0) =C ϕ n2X n=n1 k ns/2 n cos knx+θ n ,(22) ˙ϕ(x,0) =− n2X n=n1 sn ωϕ(kn) kn ∂x h Cϕ k ns/2 n cos knx+θ n i , (23) wheres n ∈ {+1,−1}selects co-/counter-propagating content. Set Cϕ = Aq 1 2 Pn2 n=n1 k ns n ,(24) so that RMSx[ϕ] =A(for r...
-
[10]
This is the cleanest way to control initial cross- correlation between sectors
Phase-correlated two-field plane waves For a single carrierk, ϕ(x,0) =Acos k(x−x ϕ) ,(25) ˙ϕ(x,0) =− ωϕ(k) k ∂xϕ(x,0),(26) χ(x,0) =A rcos k(x−x χ) + ∆ϕ ,(27) ˙χ(x,0) =−σ ωχ(k) k ∂xχ(x,0),(28) with amplitude ratior >0, relative phase ∆ϕ∈[0, π], andσ∈ {+1,−1}for co-/counter-propagation. This is the cleanest way to control initial cross- correlation between ...
-
[11]
Oscillon-like, time-symmetric seeds ϕ(x,0) =Asech x−x 0 σ , ˙ϕ(x,0) = 0,(29) χ(x,0) =A rsech x−x 0 σ cos ∆ϕ,˙χ(x,0) = 0.(30) To add a carrier, we may multiply each profile by cos(k0(x−x 0)). Oscillons are long-lived, localized, nearly periodic lumps that appear in many scalar theories [44–46]. Seed- ing an oscillon-like profile probes whether the ghostly ...
-
[12]
Each sim- ulation was run until a time step numerically diverged
Plane Wave Initial Conditions The plane wave tests sweep over the field initial am- plitudeAand wavenumber ratioC=kL/2π. Each sim- ulation was run until a time step numerically diverged. Thus, we definet long-lived as the final converged time. We see from table II that systems are much longer lived if the initial amplitude is decreased. TABLE II: Plane-wa...
-
[13]
Three widths were considered, and for each one, the amplitude was varied
Gaussian packets Gaussian packet initial conditions have tunable ampli- tudeAand widthℓ. Three widths were considered, and for each one, the amplitude was varied. Note that since k= 1/(4ℓ), and we have definedC=kL/2π, we tune Crather thanℓdirectly. The packet centers were fixed atx ϕ = 0.3Landx χ = 0.7L. We look at scenarios with co-/counter-propagating p...
-
[14]
We sets n =−1 for consistent counter propagation
Colored-Noise Spectra Colored-noise initial data were generated with different spectral tiltsn s andn 2 values. We sets n =−1 for consistent counter propagation. From table VIII, we find that a more negative tilt (ns <0) leads to earlier instabilities. Recall that a more negative tilt concentrates power in the IR range, and a more positive tilt biases tow...
-
[15]
We keep initial amplitudeA= 1 and wave number ratioC=kL/2π= 1.0 for all runs
Phase-Correlated two-field Plane Waves For the phase-correlated plane wave initial data, we vary the relative phase ∆ϕ, the amplitude ratiorbetween the two fields, and the co-/counter-propagation which is controlled byσ. We keep initial amplitudeA= 1 and wave number ratioC=kL/2π= 1.0 for all runs. From tables X and XI, we find that the long lived-ness, tl...
-
[16]
Tests were performed both with (XIII) and without (XII) an added spatial carrier (k0L/2π= 1)
Oscillon-Like, Time-Symmetric Seeds These tests explore the oscillon-like seeds characterized by widthσand amplitudeA. Tests were performed both with (XIII) and without (XII) an added spatial carrier (k0L/2π= 1). These results show us that instability is reached sooner as the width,σ, increases. FIG. 4: Phase-correlated plane waves initialization case. Th...
-
[17]
J. M. Cline, S. Jeon, and G. D. Moore, The phantom menaced: Constraints on low-energy effective ghosts, Phys. Rev. D70, 043543 (2004), arXiv:hep-ph/0311312
work page Pith review arXiv 2004
-
[18]
R. P. Woodard, Avoiding dark energy with 1/rmodi- fications of gravity, Lect. Notes Phys.720, 403 (2007), arXiv:astro-ph/0601672
work page Pith review arXiv 2007
-
[19]
R. R. Caldwell, A phantom menace? cosmological consequences of a dark energy component with super- negative equation of state, Phys. Lett. B545, 23 (2002), arXiv:astro-ph/9908168
work page Pith review arXiv 2002
-
[20]
K. S. Stelle, Renormalization of higher derivative quan- tum gravity, Phys. Rev. D16, 953 (1977)
work page 1977
-
[21]
K. S. Stelle, Classical gravity with higher derivatives, Gen. Rel. Grav.9, 353 (1978)
work page 1978
-
[22]
J. Z. Simon, Higher-derivative lagrangians, nonlocality, problems and solutions, Phys. Rev. D41, 3720 (1990)
work page 1990
-
[23]
M. Ostrogradsky, M´ emoires sur les ´ equations diff´ erentielles, relatives au probl` eme des isop´ erim` etres, Mem. Acad. St. Petersbourg6, 385 (1850)
-
[24]
The galileon as a local modification of gravity
A. Nicolis, R. Rattazzi, and E. Trincherini, The galileon as a local modification of gravity, Phys. Rev. D79, 064036 (2009), arXiv:0811.2197
work page Pith review arXiv 2009
-
[25]
Degenerate higher derivative theories beyond Horndeski: evading the Ostrogradski instability
D. Langlois and K. Noui, Degenerate higher derivative theories beyond horndeski: evading the ostrogradski in- stability, JCAP1602, 034, arXiv:1510.06930
- [26]
-
[27]
J. F. Donoghue, General relativity as an effective field theory: The leading quantum corrections, Phys. Rev. D 50, 3874 (1994), arXiv:gr-qc/9405057
work page Pith review arXiv 1994
-
[28]
Can dark energy evolve to the Phantom?
A. Vikman, Can dark energy evolve to the phantom?, Phys. Rev. D71, 023515 (2005), arXiv:astro-ph/0407107
work page internal anchor Pith review arXiv 2005
-
[29]
P. Creminelli, G. D’Amico, J. Norena, L. Senatore, and F. Vernizzi, The effective theory of quintessence: thew < −1 side unveiled, JCAP0902, 018, arXiv:0811.0827
-
[30]
C. Deffayet, S. Mukohyama, and A. Vikman, Ghosts without runaway instabilities, Phys. Rev. Lett.128, 041301 (2022)
work page 2022
-
[31]
C. Deffayet, A. Held, S. Mukohyama, and A. Vikman, Global and local stability for ghosts coupled to positive energy degrees of freedom, Journal of Cosmology and As- troparticle Physics2023(11), 031
-
[32]
V. Errasti D´ ıez, J. Gaset Rif` a, and G. Staudt, Foundations of ghost stability, Fortschritte der Physik73, 2400268 (2025), https://onlinelibrary.wiley.com/doi/pdf/10.1002/prop.202400268
-
[33]
D. R. Noakes, The initial value formulation of higher derivative gravity, Journal of Mathematical Physics24, 1846 (1983)
work page 1983
-
[34]
A. Held and H. Lim, Nonlinear dynamics of quadratic gravity in spherical symmetry, Phys. Rev. D104, 084075 (2021)
work page 2021
-
[35]
A. Held and H. Lim, Nonlinear evolution of quadratic gravity in 3 + 1 dimensions, Phys. Rev. D108, 104025 (2023)
work page 2023
-
[36]
A. Held and H. Lim, Black-hole binaries and waveforms in quadratic gravity (2025), arXiv:2503.13428 [gr-qc]
-
[37]
C. Deffayet, A. Held, S. Mukohyama, and A. Vikman, Ghostly interactions in (1 + 1)-dimensional classical field theory, Phys. Rev. D112, 065011 (2025)
work page 2025
-
[38]
S. Balay, S. Abhyankar, M. F. Adams, S. Benson, J. Brown, P. Brune, K. Buschelman, E. M. Constan- tinescu, L. Dalcin, A. Dener, V. Eijkhout, J. Faibus- sowitsch, W. D. Gropp, V. Hapla, T. Isaac, P. Jo- livet, D. Karpeev, D. Kaushik, M. G. Knepley, F. Kong, S. Kruger, D. A. May, L. C. McInnes, R. T. Mills, L. Mitchell, T. Munson, J. E. Roman, K. Rupp, P. S...
work page 2025
-
[39]
M. Anderson and J.-H. Kimn, A numerical approach to space-time finite elements for the wave equation, Journal of Computational Physics226, 466 (2007)
work page 2007
-
[40]
D. A. French and T. E. Peterson, A continuous space- time finite element method for the wave equation, Math. Comput.65, 491–506 (1996)
work page 1996
-
[41]
C. Cherubini and S. Filippi, Using femlab for gravita- tional problems: numerical simulations for all, Journal- Korean Physical Society49(2005)
work page 2005
-
[42]
C. Cherubini, F. Federici, S. Succi, and M. P. Tosi, Ex- cised acoustic black holes: The scattering problem in the time domain, Phys. Rev. D72, 084016 (2005)
work page 2005
- [43]
- [44]
-
[45]
C.-K. Kim, On the Numerical Computation for Solv- ing the Two-Dimensional Parabolic Equations by Space- Time Finite Element Method, JSME International Jour- nal Series B44, 434 (2001)
work page 2001
-
[46]
M. Guddati and J. Tassoulas, Space-time finite elements for the analysis of transient wave propagation in un- bounded layered media, International Journal of Solids and Structures36, 4699 (1999)
work page 1999
-
[47]
B. Dyniewicz, Space-time finite element approach to gen- eral description of a moving inertial load, Finite Elem. Anal. Des.62, 8–17 (2012)
work page 2012
-
[48]
M. Zank, Efficient direct space-time finite element solvers for the wave equation in second-order formulation, J. Sci. Comput.105, 10.1007/s10915-025-03038-1 (2025)
-
[49]
A. Schwing, I. Nompelis, and G. V. Candler, Im- plementation of adaptive mesh refinement in an im- plicit unstructured finite-volume flow solver, in21st AIAA Computational Fluid Dynamics Conference, https://arc.aiaa.org/doi/pdf/10.2514/6.2013-2446
-
[50]
X. Xu, Y. Chen, Z. Han, and F. Zhou, A total energy- based adaptive mesh refinement technique for the simu- lation of compressible flow, Frontiers in Energy Research Volume 11 - 2023, 10.3389/fenrg.2023.1203801 (2023). [35]Adaptive Mesh Refinement for DDES Sim- ulation on Transonic Compressor Cas- cade With Unstructured Mesh, Turbo Expo, Vol. Volume 2C: T...
-
[51]
G. L. Bryan, M. L. Norman, B. W. O’Shea, T. Abel, J. H. Wise, M. J. Turk, D. R. Reynolds, D. C. Collins, P. Wang, S. W. Skillman, B. Smith, R. P. Harkness, J. Bordner, J.-h. Kim, M. Kuhlen, H. Xu, N. Goldbaum, C. Hummels, A. G. Kritsuk, E. Tasker, S. Skory, C. M. Simpson, O. Hahn, J. S. Oishi, G. C. So, F. Zhao, R. Cen, and Y. Li, Enzo: An adaptive mesh r...
work page 2014
-
[52]
G. Xu, Hydrodynamic and n-body schemes on an un- structured, adaptive mesh with applications to cosmo- logical simulations, Monthly Notices of the Royal Astro- nomical Society288, 903–919 (1997)
work page 1997
-
[53]
E. Evans, S. Iyer, E. Schnetter, W.-M. Suen, J. Tao, R. Wolfmeyer, and H.-M. Zhang, Computa- tional relativistic astrophysics with adaptive mesh refine- ment: Testbeds, Physical Review D71, 10.1103/phys- revd.71.081301 (2005)
-
[54]
Nazarenko,Wave Turbulence, Lecture Notes in Physics, Vol
S. Nazarenko,Wave Turbulence, Lecture Notes in Physics, Vol. 825 (Springer, 2011)
work page 2011
-
[55]
P. Walczak, S. Randoux, and P. Suret, Optical rogue waves in integrable turbulence, Phys. Rev. Lett.114, 143903 (2015)
work page 2015
-
[56]
S. Randoux and P. Suret, Integrable turbulence: a review of recent results in optics (2016), preprint
work page 2016
- [57]
- [58]
-
[59]
M. Gleiser and D. Sicilia, General theory of oscillon dy- namics, Phys. Rev. D80, 125037 (2009)
work page 2009
-
[60]
M. A. Amin and D. Shirokoff, Flat-top oscillons in an expanding universe, Phys. Rev. D81, 085045 (2010)
work page 2010
-
[61]
M. Hindmarsh and P. Salmi, Oscillons and domain walls, Phys. Rev. D77, 105025 (2008). 16 Appendix A: Element Stiffness Matrix Calculations An important step in any FEM is determining the el- ement stiffness matrices. These matrices are found by solving the weak form of the equations of motion, Eq
work page 2008
-
[62]
Solving the space-time FEM for the (1 + 1) case re- sults in 4x4 matrices, the (2 + 1) case finds 8x8 matrices, and the 3+1 case has 16x16 matrices. The weak equations are displayed in equation 20, but in equations A1, A2, A3, and A4 we display them in their (1 + 1) form. K1 = Z X,T utΨ +ϕ xΨx +m 2 ϕϕΨ +V ϕΨ dxdt(A1) K2 = Z X,T (ϕtΨ−uΨ)dxdt(A2) G1 = Z X,T...
-
[63]
A5, we con- sider the four corners of a rectangle in the (x, t) plane, see Fig
Element Basis Function The rectangular element basis function is a piecewise polynomial with four terms, Ψi(x, t) =b 1,ix+b 2,it+b 3,ixt+b 4,i.(A5) To solve for the unknown coefficients in Eq. A5, we con- sider the four corners of a rectangle in the (x, t) plane, see Fig. 11. (0,0) (hx,0) (0,ht) (hx,ht) FIG. 11 In figure 11,h x andh t represent the step s...
-
[64]
Element Stiffness Matrices Now that we have the basis functions, the element stiff- ness matrices can be determined. We will explain the set up of the element stiffness matrices, display the matri- ces, and then discuss practical implementation into the simulation. 17 In the two dimensional (1 + 1) case, the weak form of the equations of motion, equations...
-
[65]
Here,λis a parameter controlling the strength of the nonlinear potential
Manufactured Solution Tests We consider the following coupled partial differential equations (PDEs) in (1 + 1) dimensions: ϕtt −ϕ xx +ϕ+V ϕ(ϕ, χ) = 0,(B1) χtt −χ xx +χ−V χ(ϕ, χ) = 0,(B2) where the highly nonlinear potential terms are defined as Vϕ(ϕ, χ) =−2λ ϕ A B1.5 Vχ(ϕ, χ) = 2λ χ C B1.5 with A=ϕ 2 −χ 2 + 1 B= ϕ2 −χ 2 −1 2 + 4ϕ2, C=ϕ 2 −χ 2 −1. Here,λis...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.