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Liquidation with self-exciting price impact

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Abstract

We study optimal execution with “self-exciting” price impact, where persistent trades not only incur price impact but also increase the execution costs for successive orders. This model is motivated by an equilibrium between fundamental sellers, market makers, and end users. For risk-neutral investors, it leads to faster initial trading compared to the constant execution rate of Bertsimas and Lo [5]. For risk-averse liquidation as in Almgren and Chriss [2, 3] or Huberman and Stanzl [15], self-excitement has a moderating effect: slow liquidation is sped up, whereas fast schedules are slowed down.

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Notes

  1. Front running becomes optimal in the presence of sufficiently large “preys” in the models of Brunnermeier and Pedersen [6] as well as Carlin, Lobo, and Viswanathan [7]. In the model of Schied and Schöneborn [20], potential predators can be either detrimental or beneficial depending on the model parameters.

  2. Very similar models were proposed and studied concurrently by Bertsimas and Lo [5], Madhavan [18], as well as Huberman and Stanzl [15]. To keep in line with most of the literature, we nevertheless stick to the nomenclature “Almgren–Chriss model”.

  3. Recently, a different kind of “self-excitement” has also started to receive increasing attention, see, e.g., [1] and the references therein. In these models, the orders of other market participants are modeled by a Hawkes process, a counting process whose jump intensities are self-exciting in that they are influenced by the past jumps. Whence, self-excitement is produced by the trades of the other market participants in these models, whereas it is instigated by the large trader in ours.

  4. Since time horizons for liquidation programs are typically short, drifts are usually neglected (but cf. [16]) and it is reasonable to work with more tractable arithmetic Brownian motions rather than their geometric counterparts (but cf. [9]). In the case of a risk-neutral investor, the price process need not be an arithmetic Brownian motion, but can be a general martingale.

  5. This price impact is purely temporary, in that it only affects the current trade but not subsequent ones. Linear permanent price impact can also be accounted for by shifting the unaffected price quote, see [3]. However, like proportional transaction costs, linear permanent impact does not alter optimal execution strategies. Hence, we disregard these two frictions throughout. Nonlinear permanent price impact depending on the cumulated number of shares sold by the large trader is studied by [13].

  6. The linear dependence is assumed for tractability. It allows for closed-form solutions and also can be seen as a first-order approximation for more general small self-excitement mechanisms.

  7. Indeed, assume we start with X shares. Buying shares at a constant rate on the interval \([0,\frac{T}{2}]\) to reach \(X+\frac{\ell _0}{\ell _1}+k\), for some integer k, and selling back these shares at the same speed on \([\frac{T}{2},T]\) yields an expected profit of order \(O(k^3)\) as k grows to infinity, while the standard deviation of the final profit is of order O(k).

  8. To allow for buy orders in our model and rule out price manipulations, we could define the price impact parameter as \(\lambda _t:=\ell _0 + \ell _1 (X-x_t)^+\) when selling (\(\dot{x}_t<0\)) and \(\lambda _t:=\ell _0\) when buying (\(\dot{x}_t > 0\)). This means that, during a substantial liquidation, sales increase the price impact of further sales whereas the price impact of purchases remains constant. In such a model round-trips have a strictly positive expected cost, and optimal strategies are necessarily decreasing.

  9. For convenience, we assume that \(h/\Delta t\) is an integer.

  10. Here, the risk-free rate is set equal to zero, because the time horizons we consider are short.

  11. Note, however, that there is recent empirical evidence suggesting that the marginal impact of child orders decreases as metaorder execution proceeds [4, 12]. Whence, the argument presented here may only apply for very large execution programs.

  12. Adaptive strategies are studied by Almgren and Lorenz [17] for a mean-variance criterion and by Schied and Schöneborn [19] for von Neumann-Morgenstern utilities. Here, we focus on deterministic strategies to obtain tractable solutions also with our more complicated price impact structure in Sect. 4.2. In the risk-neutral case, this entails no loss of generality, cf. Remark 4.2.

  13. The integrand to be minimized pointwise for each \(t\in [0,T]\) is given by \(F\left( t,x,v\right) = (\ell _0+\ell _1 X)v^2 -\ell _1 x v^2 \); its Hessian is \( \left( {\begin{array}{l@{\quad }l} 0 &{}\quad { - 2\ell _{1} v} \\ { - 2\ell _{1} v} &{}\quad {2\left( {\ell _{0} + \ell _{1} \left( {X - x} \right) } \right) } \\ \end{array} } \right) \) . The sum of this matrix’ eigenvalues is positive for \(x\in [0, X]\) and their product negative. Whence the goal functional is not convex.

  14. Note that for \(\ell _1=0\), we recover the Euler–Lagrange equation (4.1) in the classical Almgren–Chriss model. Conversely, for \(\ell _1>0\) but \(\gamma =0\) we are back in the risk-neutral setting of Sect. 4.2.

  15. Indeed, an inspection of the explicit formula shows that this holds uniformly on [0, T], so that the claim for the remainder follows from the dominated convergence theorem.

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Acknowledgments

We thank Pierre Collin-Dufresne for fruitful discussions in the initial stages of the project. We are also grateful to two anonymous referees and an anonymous associate editor for numerous constructive comments.

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Correspondence to Johannes Muhle-Karbe.

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Partially supported by the ETH Foundation.

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Cayé, T., Muhle-Karbe, J. Liquidation with self-exciting price impact. Math Finan Econ 10, 15–28 (2016). https://doi.org/10.1007/s11579-015-0148-2

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