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Marketron games: Self-propelling stocks vs dumb money and metastable dynamics of the Good, Bad and Ugly markets

T0 review · 4 major / 5 minor · reviewed 2026-08-10 · deepseek-v4-flash

Pith's one-line read A money-flow feedback loop can generate three metastable market regimes, including crashes and defaults, without jumps or separate default processes.

desk verdict A genuinely new 2D marketron model with memory and real calibration effort, but the three-regime claim is enforced by constraints whose derivation fails at the fitted parameters. read the letter →

arxiv 2501.12676 v2 pith:QJGZ37DY submitted 2025-01-22 q-fin.MF q-fin.CP

classification q-fin.MFq-fin.CP MSC 91G8060H1082C31
keywords marketroninelasticmarkethypothesisdumbmoneyeffectmetastablemarketsinstantontransitionsdefaultableequityLangevindynamicsactivematter
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

This paper builds a model of price formation in an inelastic market where the only structural ingredients are money flows, their price impact, and unobservable predictive signals. It claims that feedback between market performance and new-money flows creates a nonlinear potential landscape with three metastable states: a Good market, a Bad market, and an Ugly collapse or default state. Crashes and defaults are described as instanton transitions of a 'marketron' particle over potential barriers, so no exogenous jump process or separate default mechanism is needed. Calibrated to S&P500 monthly log-prices from 2000 to 2024, the model matches the first four moments of log-returns and produces an annualized default intensity of about 18 basis points, inside the 10-50 basis point range inferred from credit markets. If this is correct, defaults are implicit in ordinary equity dynamics rather than added on top of them.

What carries the argument

The machinery is the marketron potential $V(x,y)=-\eta x + c(t)y\,V_M(x)+\frac{1}{2\mu}(y-\bar y)^2$, whose $x$-gradient drives the log-price and whose $y$-gradient drives the memory variable. The flow potential $V_M(x)$ is approximated by an inverted Morse potential, and in the D-limit of zero noise, zero signal, and short memory the memory variable is slaved to $x$, leaving the effective one-dimensional potential $U_{\rm eff}(x)=-\eta x + c(t)\bar y\,V_M(x)-\frac{c(t)^2}{2\mu}V_M^2(x)$. Appendix C imposes constraints on the quartic $zV'(z)$ to guarantee four real roots and hence three extrema, which are the Good, Bad, and Ugly states. Instantons, defined as trajectories of the inverted potential that dominate the weak-noise path integral, convert barrier crossings into fast transitions between these metastable states, which is what makes crashes and defaults rare but possible.

What would settle it

Recalibrate Eq. (29) to S&P500 daily returns without imposing the Appendix C constraints; if a moment-matching solution exists whose potential has fewer than three extrema, or whose simulated default intensity falls far outside the 10-50 basis point range, then the three-regime metastable structure and the 18 basis point default reading are consequences of the constraints rather than of the money-flow mechanism.

Watch

Extended reading notes

Core claim

The central claim is that price dynamics in an inelastic market can be represented as nonlinear diffusion of a marketron in a two-dimensional potential $V(x,y)=-\eta x + c(t)y\,V_M(x)+\frac{1}{2\mu}(y-\bar y)^2$, where $x$ is the log-price and $y$ is a memory variable storing past money flows. When money flows respond positively to market performance, the coupling between $y$ and the inverted-Morse flow potential creates barriers, so the potential has three extrema. The right minimum is the Good market, the middle minimum is the Bad market, and the maximum with an escape route to $x\to-\infty$ is the Ugly market. Transitions between these states are instanton solutions of the flipped-potential dynamics, making the regimes metastable. Calibrating the three-dimensional version to S&P500 monthly log-prices under shape constraints reproduces the skewness and kurtosis of log-returns and produces defaults at a rate of about 18 basis points, which the paper presents as evidence that defaultability emerges from money-flow feedback rather than from an added jump process.

Load-bearing premise

The load-bearing premise is that the small-noise memory-variable approximation behind the constraints in Eq. (30) is accurate enough that forcing the quartic $zV'(z)$ to have four real roots genuinely yields the Good/Bad/Ugly landscape rather than an artifact; if the $y$-noise is strong, those constraints become stochastic and the calibrated three-regime structure is no longer guaranteed.

Editorial extensions

If this is right

  • Equity defaults and market crashes require no jump process or exogenous default intensity; they arise as instanton escapes through barriers created by the money-flow feedback loop.
  • The calibrated model reproduces the negative skew and positive excess kurtosis of S&P500 log-returns across horizons from 2 to 24 years.
  • Simulated paths of the calibrated model generate an annualized default intensity near 18 basis points, within the 10-50 basis point range inferred from credit markets, using only equity data.
  • Because the model is Markovian in $(x,y,\theta)$ but non-Markovian in price alone, volatility clustering and price-volatility correlations emerge from the memory variable rather than from an external stochastic-volatility process.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • Pith inference: The model turns equity and credit into two readings of one parameter set; joint calibration to equity returns and CDS spreads could tighten the 10-50 basis point default intensity band and test the physical-to-credit link.
  • Pith inference: Treating the unobservable OU signals as self-propulsion suggests that optimal investor policies could be derived as minimum-cost controls of an active particle in the Good/Bad/Ugly landscape, not merely calibrated.
  • Pith inference: A direct test would replace the shape constraints with unconstrained calibration to daily returns and check whether three extrema persist; if they disappear, the metastable structure is an artifact of the constraints rather than a prediction.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

4 major / 5 minor

Summary. This paper proposes a two-dimensional Langevin ('marketron') model of price formation in which the log-price x and a memory variable y evolve under a potential V(x,y) = -ηx + c(t)y V_M(x) + (1/(2μ))(y - ȳ)^2 (Eqs. 18 and 20). The memory variable encodes past money flows, and an unobserved OU signal z is reinterpreted as an active self-propulsion force. In the D-limit μ >> 1 the model reduces to a 1D effective potential (Eq. 26) and is claimed to produce three metastable market regimes—Good, Bad, Ugly—with instanton transitions. The model is calibrated to S&P 500 monthly log-returns using a particle filter with shape constraints (Eq. 30); the calibrated model matches the first four moments of log-returns across horizons and produces an annualized default intensity of about 18 bps without exogenous jumps.

Significance. If the three-regime landscape were emergent, the paper would be a substantial contribution: it offers a parsimonious nonlinear mechanism for crashes and defaults, connects flow impact to metastability, and provides a transparent calibration with explicit parameters, seeds, and constraints. The strengths include the internally consistent 2D potential algebra, the explicit reporting of all 18 calibrated parameters in Tables 1 and 4, and the reproducible calibration protocol. However, the empirical identification of the three regimes is undermined by the fact that the constraints in Eq. (30) are imposed during calibration, and the approximations used to derive them are violated by the calibrated parameters. The 18 bps default intensity can therefore not yet be read as an independent confirmation of the metastable landscape.

major comments (4)
  1. [§6, Appendix C, Eq. (30)] The three-regime structure is enforced, not predicted. The text states that the constraints 'explicitly require the calibrated parameters to preserve the necessary shape', and Eq. (30) are derived in Appendix C as necessary conditions for the quartic zV'(z) to have four real roots. Figures 16 and 17 therefore show only that the calibration constraints were satisfied. To support the claim that the model 'predicts' Good/Bad/Ugly regimes, please add an unconstrained calibration and report the shape of the resulting potential, or explicitly reframe the regime structure as part of the model specification and revise the abstract and Section 7 accordingly.
  2. [Appendix C, Eq. (C.12)] The stochastic correction to the constraints is invalid. The derivation drops σ_y from the y-SDE; with σ_y > 0, y(0) is replaced by y(0) - σ_y∫... in Eq. (C.11). The assertion in Eq. (C.12) that y(0) >> σ_y times the martingale is 'always true on average' does not hold: since the calibration sets y(0) = 0 (Section 6.2), the required inequality is M_t << 0, and a zero-mean martingale does not satisfy this almost surely. Moreover, Table 1 gives σ_y = 0.38, comparable to σ = 0.79, so the small-noise premise is violated. Consequently, the calibrated parameters do not provably yield a three-extremum potential in the full stochastic model.
  3. [§3.1, Eq. (25)] The D-limit approximation (Eq. 25) requires μ >> 1, but the qualitative figures (Figs. 2-6) use μ = 0.1, and the calibrated values are μ = 1.67 and μ = 1.40 (Tables 1 and 4). The 1D potential U_eff (Eq. 26) and the Good/Bad/Ugly taxonomy derived from it are therefore not justified for these parameters. Please quantify the error of the D-limit at the calibrated parameters, for example by comparing 1D and 2D stationary densities or escape rates.
  4. [§6.2.1, default intensity] The annualized default intensity of about 18 bps is obtained from Monte Carlo simulation of the full 3D model using parameters selected under the constraints of Eq. (30). Given the issues with Eq. (C.12) and the small-noise premise, this number does not by itself validate the metastable barrier picture. Please compute the default intensity with unconstrained parameters, or at least verify the four-root condition with the full stochastic y-process, and report the resulting intensity.
minor comments (5)
  1. [Section 6.2] The sentence 'we use x0 = x(0), θ0 = y(0) = 0, y0 = y(0)' is ambiguous about the initial values; please state y0 and θ0 separately and consistently with Eq. (C.12).
  2. [Eq. (C.12)] The integrand is written with ε_t inside an integral over k; the noise should depend on the integration variable (e.g., ε_k), and the integral should be defined precisely.
  3. [Footnote 7] The inequality '0≥S≤∞' should read '0≤S≤∞'.
  4. [Table 3] The table labels kurtosis as 'annualized', but excess kurtosis is scale-invariant in this context; please clarify the reported quantity.
  5. [References] The reference 'Alt-Sahalia, Y.' should be 'Aït-Sahalia, Y.'.

Circularity Check

2 steps flagged · score 8.0 of 10

Three 'predicted' market regimes are imposed by the Eq. (30) calibration constraints; the Appendix C stochastic correction used to justify them is asserted away with an invalid martingale bound.

  1. self definitional [Section 6, Eq. (30); Section 6.2.1 'The marketron potential shape' (Figs. 16-17)]
    "Since this paper is focused on situations where the marketron potential has a form as in Fig. 6 (where transitions between various regimes occur via the instanton mechanism), additional constraints should be imposed when performing filtering because not every calibration gives rise to this form of potential. ... By adding an additional constraint as in Appendix C, we explicitly require the calibrated parameters to preserve the necessary shape. ... Accordingly, the potential has three extrema, i.e., exactly what we tried to achieve."

    The three-regime landscape is not an emergent output of the model: the optimizer is explicitly constrained to the region of parameter space where zV'(z) has four real roots, which is exactly the condition for the potential to have three extrema. The paper's own words confirm this ('we explicitly require the calibrated parameters to preserve the necessary shape' and 'exactly what we tried to achieve'). Any feasible solution of the constrained calibration therefore displays Good/Bad/Ugly structure by construction. The abstract's claim that the model 'predicts three distinct regimes' is thus a restatement of the imposed constraints, not an independent prediction.

  2. other [Appendix C, Eqs. (C.11)-(C.12)]
    "In this case the constraint in Eq. (C.9) becomes stochastic, and it is not obvious how it can be used in the filtering method. Therefore, we impose an additional constraint that reads y(0)≫σy∫t0 ekµϵtdk = σy(Wteµt−1µ∫t0 Wkekµdk). The RHS of this inequality is a martingale, therefore, on average, it is always true."

    This assertion is used to justify neglecting the y-noise when deriving the four-root constraints of Eq. (30). But the RHS is a zero-mean martingale, so its expectation is zero at every t; with the calibration's y(0)=0, the inequality 0 ≫ 0 is false on average, not 'always true'. The phrase 'on average' cannot control the pathwise magnitude of the noise that enters the actual filter. Since Eq. (30) is the only mechanism that enforces the three-extrema landscape, and the calibrated σy=0.38 is comparable to σ=0.79 (Table 1), the central regime claim rests on a stochastic correction that is asserted away rather than derived.

full rationale

The Langevin construction in Eqs. (12)-(23) is internally coherent as a model specification, and the calibration to S&P500 moment data is a legitimate fitting exercise. The circularity is concentrated in the paper's central claim. Section 6 explicitly constrains calibration to parameters that preserve a three-extrema potential shape, and Section 6.2.1 then reports the presence of three extrema as the result the authors 'tried to achieve.' The 18 bps default intensity and metastable regime dynamics are simulated with this enforced landscape, so they do not independently validate the Good/Bad/Ugly prediction. Appendix C's attempt to extend the four-root constraints beyond small y-noise fails because the inequality y(0)≫(zero-mean martingale) is not 'always true on average'—especially with y(0)=0 and σy=0.38. No load-bearing self-citation chain was found; prior Halperin/Dixon work is used as modeling background, not as a uniqueness theorem. Overall, the central 'prediction' is better described as a constrained calibration result, meriting a circularity score of 8.

Assumptions & free parameters 10 free parameters · 7 assumptions · 2 invented entities

The central claim depends heavily on the fitted parameters of the posited policy and impact functions, and on the constraints that force the potential to have three extrema. The memory variable and the marketron are introduced as latent or conceptual entities without independent falsifiable handles.

free parameters (10)
  • g (coupling constant) = 0.6831 (Table 1)
    Couples investor money flow to market performance; creates the potential barrier when g>0. Central to the regime structure.
  • c (money flow scale) = 3.9305 (Table 1)
    Scales the money flow rate and the strength of the impact term in the potential.
  • mu (memory depth) = 1.6671 (Table 1)
    Sets the relaxation rate of the memory variable y; controls the D-limit approximation and the potential curvature.
  • ybar (threshold) = 0.4731 (Table 1)
    Defines the level at which past flows saturate the impact; the 'dumb money' threshold.
  • eta (risk-adjusted drift) = -1.5685 (Table 1)
    Combines risk-free rate and volatility; negative values allow escape to negative infinity (default).
  • sigma, sigma_y, sigma_z (noise levels) = 0.7912, 0.3800, 0.8334 (Table 1)
    Volatilities of the log-price, memory, and signal processes; calibration parameters.
  • k (mean reversion of signal) = 1.2869 (Table 1)
    Speed of reversion of the hidden OU signal theta.
  • thetabar (signal mean level) = 6.7865 (Table 1)
    Long-term mean of the hidden OU signal.
  • b1, b2, k1x, k2x, k3x, k1y, k2y, k3y (signal shape parameters) = Various, Table 1
    Parameters of the functions f and h that convert the signal into drift; 8 additional degrees of freedom.
  • epsilon (regularization parameter) = 0.02 (fixed, Section 6.2)
    Set by hand to regularize the policy at small prices; not calibrated but affects the potential.
assumptions (7)
  • standard math Itô's lemma and standard stochastic calculus are used to transform the price SDE into log-price dynamics.
    Invoked in Section 2 when deriving Eq. (4).
  • domain assumption The investor policy ut = c(t) S0 [1 - g/(e^x + epsilon g)] is a posited functional form, not derived from utility optimization.
    Section 2.2, Eq. (9). The regime structure depends on this policy.
  • ad hoc to paper The price impact function I = y_t u_t/S_t with memory variable y_t is assumed, and the potential V(y) is chosen so that the y-dynamics reproduce an EMA of flows.
    Section 2.3 and Eq. (17). Reverse-engineered to match a desired Langevin form.
  • domain assumption Return predictors are unobservable OU processes (Eq. 6), interpreted as self-propulsion; this interpretation does not change the mathematics but is presented as the active matter analogy.
    Section 2.1 and 5.2.
  • ad hoc to paper The calibration imposes the shape constraints in Eq. (30) which guarantee four roots of the quartic, hence three extrema of the potential.
    Appendix C and Section 6. These constraints force the Good/Bad/Ugly landscape.
  • ad hoc to paper The D-limit approximation y_t = ybar + (c/mu) V_M(x) assumes mu >> 1, but is used with mu = 0.1 in qualitative plots.
    Eq. (25) and figures in Section 3 use parameters outside the assumed limit.
  • domain assumption The approximate inverted-Morse potential Eq. (19) is used for qualitative analysis and in the constraint derivation.
    Section 3 and Appendix C; the exact potential differs at x -> -inf, which the authors acknowledge.
invented entities (2)
  • Memory variable y_t
    purpose: Latent state tracking past money flows to produce the dumb money saturation effect and non-Markovian price dynamics.
    y is unobservable and only estimated through particle filtering; no direct falsifiable prediction outside the model.
  • Marketron quasi-particle
    purpose: Conceptual name for the 2D diffusion (x,y) in the potential; aids the active matter analogy.
    It is a renaming of the stochastic process, not a new physical entity, and has no external measurable handle.

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Pith. "Pith review of Marketron games: Self-propelling stocks vs dumb money and metastable dynamics of the Good, Bad and Ugly markets." pith.science (2026). https://pith.science/paper/QJGZ37DY

@misc{pith2026250112676,
  author       = {Pith},
  title        = {Pith review of: Marketron games: Self-propelling stocks vs dumb money and metastable dynamics of the Good, Bad and Ugly markets},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/QJGZ37DY}},
  note         = {Machine review of arXiv:2501.12676}
}
abstract

We present a model of price formation in an inelastic market whose dynamics are partially driven by both money flows and their impact on asset prices. The money flow to the market is viewed as an investment policy of outside investors. For the price impact effect, we use an impact function that incorporates the phenomena of market inelasticity and saturation from new money (the $dumb \; money$ effect). Due to the dependence of market investors' flows on market performance, the model implies a feedback mechanism that gives rise to nonlinear dynamics. Consequently, the market price dynamics are seen as a nonlinear diffusion of a particle (the $marketron$) in a two-dimensional space formed by the log-price $x$ and a memory variable $y$. The latter stores information about past money flows, so that the dynamics are non-Markovian in the log price $x$ alone, but Markovian in the pair $(x,y)$, bearing a strong resemblance to spiking neuron models in neuroscience. In addition to market flows, the model dynamics are partially driven by return predictors, modeled as unobservable Ornstein-Uhlenbeck processes. By using a new interpretation of predictive signals as $self$-$propulsion$ components of the price dynamics, we treat the marketron as an active particle, amenable to methods developed in the physics of active matter. We show that, depending on the choice of parameters, our model can produce a rich variety of interesting dynamic scenarios. In particular, it predicts three distinct regimes of the market, which we call the $Good$, the $Bad$, and the $Ugly$ markets. The latter regime describes a scenario of a total market collapse or, alternatively, a corporate default event, depending on whether our model is applied to the whole market or an individual stock.

Figures

Figures reproduced from arXiv: 2501.12676 by the authors.

Figure 1
Figure 1. Combined inflows into equity, bond, and hybrid funds. The annual rate is approximately constant at the level of $325bn, [Deutsche Bank Security Inc., 2016]. Second, we want the impact function to capture the "dumb money" effect, [Frazzini and Lamont, 2008], which amounts to diminishing stock returns once the cumulative money flow into the stock over some period of time (of the order of one year) exceeds some critica… view at source ↗
Figure 2
Figure 2. The marketron potential Eq. (20) as a function of the log-price x and the memory variable y, for η < 0. Parameters’ values are: c(t) = 0.13, g = 0.3, µ = 0.1, y¯ = 1., η = −0.01. The landscape of the marketron potential describes possible market regimes (see the main text). This is simply an OU process with a stochastic mean reversion level that also depends on xt . Integrating this SDE while omitting the signal z (… view at source ↗
Figure 3
Figure 3. Contour plots of the marketron potential Eq. (20) for η < 0 and η > 0. Parameters’ values are: c(t) = 0.13, g = 0.25, µ = 0.1, y¯ = 1., η = −0.01. When η < 0, the particle placed in the local minimum will escape to the low right corner by barrier crossing. For η > 0, there is also an option to escape to the region x → ∞, shown as an additional red dot on the top. marketron potential becomes a linearly increasing fun… view at source ↗
Figures from the paper (18 more)
Figure 4
Figure 4. Figure 4: The marketron potential Eq. (20) as a function of x with η < 0 for fixed values of y. Parameter values are: c(t) = 0.13, g = 0.25, µ = 0.1, y¯ = 1., η = −0.01. When y > 0, the potential enables escape either to x → −∞ or to x → ∞ through a barrier whose height grows wi…
Figure 5
Figure 5. Figure 5: The effective 1D marketron potential Eq. (26) with various values of η. Larger values of η mimic the effect of an increasing active signal zt on the overall dynamics via η¯. If η is negative, the particle can escape to the negative infinity via instantons, see Section …
Figure 6
Figure 6. Figure 6: On the left: Ueff(x) from [PITH_FULL_IMAGE:figures/full_fig_p017_6.png]
Figure 7
Figure 7. Figure 7: Instanton solutions describing transitions from the Bad to the Good market (on the left), and from the Good to the Bad market (on the right). the relationship between market performance and money flows - specifically, that money tends to flow more readily into well-per…
Figure 8
Figure 8. Figure 8: Autocorrelation of a) S&P500 daily returns, and b) the squared returns. computed using this time series. The serial correlation is small for all lags except lag one. The mean correlation is close to zero, and the correlation does not show any significant nonrandom vari…
Figure 9
Figure 9. Figure 9: Plot of log-returns computed by using the market data and by the marketron model with the model parameters found by calibration. of approximately 18 bps, which aligns well with market-implied default intensities ranging from 10 to 50 bps based on credit market data. 5 …
Figure 10
Figure 10. Figure 10: Skewness and kurtosis as functions of time with the calibrated marketron model for a) log-returns xt, and b) the memory variable yt. Distributions of the model variables. The next set of plots presents distributions of variables xt , yt obtained in the simulation [PI…
Figure 11
Figure 11. Figure 11: The Q-Q plots of xt computed vs the normal distribution for different time horizons, obtained by simulation. 2.0 1.5 1.0 0.5 0.0 0.5 1.0 1.5 2.0 0 10 20 30 40 50 Count 12 120 240 [PITH_FULL_IMAGE:figures/full_fig_p026_11.png]
Figure 12
Figure 12. Figure 12: The distributions of the log-prices x at t = 1, 10, 20 years obtained by simulation. Thus, nonlinearities in the drift for variables xt and yt give rise to skewed distributions of these variables. Therefore, the results obtained with the full marketron model qualitati…
Figure 13
Figure 13. Figure 13: The distributions of the memory variable y at t = 1, 10, 20 years, obtained by simulation. The annualized realized volatility [PITH_FULL_IMAGE:figures/full_fig_p027_13.png]
Figure 14
Figure 14. Figure 14: Annualized realized volatility of log-prices xt along several paths, obtained by simulation of Eq. (29) with calibrated parameters. To quantify these observations, we computed the Hurst exponent H of the volatility of log-returns obtained in our experiment. In agreeme…
Figure 15
Figure 15. Figure 15: Annualized realized volatility of yt along several paths, obtained by simulation of Eq. (29) with calibrated parameters. The marketron potential shape. To ensure these parameters produce the marketron potential of the expected shape, we plot the function zV ′ (z) (as …
Figure 16
Figure 16. Figure 16: Plot of zV ′ (z) as defined in Eq. (C.5) at t = 0.1: a) the zoomed-in picture to see two real roots close to the origin; b) the other two roots. It can be seen in [PITH_FULL_IMAGE:figures/full_fig_p028_16.png]
Figure 17
Figure 17. Figure 17: Plot of zV ′ (z) as defined in Eq. (C.5) at t = 1: a) the zoomed-in picture to see two real roots close to the origin; b) the other two roots. 2 1 0 1 2 3 4 2 x 0 2 y 4 150 100 50 0 50 100 150 200 150 100 50 0 50 100 150 200 (a) 2 1 0 1 2 3 4 2 x 0 2 y 4 150 100 50 0 …
Figure 18
Figure 18. Figure 18: 3D marketron potential V (x, y) in Eq. (15) computed with the model parameters found by calibration for a) t = 1 year, b) t = 20 years. found by calibration for times t = 1, 20 years. In agreement with Figs. 16 and 17 and the discussion in Section 3.1, these results c…
Figure 19
Figure 19. Figure 19: Three months moments of log-returns obtained by using the market and model data: a) mean, b) skew, c) kurtosis, and d) volatility. of daily historical data (approximately 60 points) with three years of monthly historical data (39 points). While this sample size is not…
Figure 20
Figure 20. Figure 20: 3D marketron potential V (x, y) in Eq. (15) computed with the model parameters found by calibration for a) t = 1 year, b) t = 20 years, θ∗ = ˆθ. converges to different solutions depending on the random noise realization, while still maintaining good agreement with mar…
Figure 21
Figure 21. Figure 21: Approximation of the marketron potential by a piecewise harmonic potential. discussion in [Itkin, Lipton, and Muravey, 2022] and references therein), this gives rise to the process in Eq. (27) to be driven by a skewed Brownian Motion instead of a normal one. Thus, the…

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Works this paper leans on

3 extracted references · 3 canonical work pages · cited by 1 Pith paper

  1. [1]

    If ∆> 0 and P <0,D< 0, then all four roots are real and distinct

  2. [2]

    If ∆ = 0 and P <0,D< 0, ∆0̸= 0, then there are a real double root and two real simple roots

  3. [3]

    Computing the RHS of Eq

    If ∆< 0 there are two distinct real roots and two complex conjugate roots. Computing the RHS of Eq. (C.7) with allowance for the definitions in Eq. (C.6) yields ∆ = 1 16c(t)3g2J(t) { c(t)3g2I(t)4[J(t)− 2gI(t)] + 16c(t)¯η2g2J(t) [ −2g2I(t)2− 2gI(t)J(t) +J(t)2 ] − 4c(t)¯η [ c(t)g4I(t)4 + 2g2I(t)2J(t) [3c(t)gI(t) + 2] + 8J(t)3 [3c(t)gI(t) + 2] (C.9) + 2gI(t)...

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