M2-M5 blackfold funnels

We analyze the basic M2-M5 intersection in the supergravity regime using the blackfold approach. This approach allows us to recover the 1/4-BPS self-dual string soliton solution of Howe, Lambert and West as a three-funnel solution of an effective fivebrane worldvolume theory in a new regime, the regime of a large number of M2 and M5 branes. In addition, it allows us to discuss finite temperature effects for non-extremal self-dual string soliton solutions and wormhole solutions interpolating between stacks of M5 and anti-M5 branes. The purpose of this paper is to exhibit these solutions and their basic properties.


M2-M5
The star of this short note is the M2-M5 intersection in IR 1,10 . This setup, which is 1/4-BPS at extremality, is interesting for a variety of reasons.
The (1+1)-dimensional intersection is a self-dual string whose properties underlie many of the mysteries of the M2 and M5 brane physics and M-theory itself (for a relevant review we refer the reader to [1]). In the past it has been studied from several points of view: (1) As a supersymmetric soliton solution of the effective fivebrane worldvolume theory of a single M5 brane [2]. The solution, which preserves the requisite SO(1, 1) × SO(4) × SO(4) symmetry, has a non-trivial worldvolume self-dual three-form flux and a single non-trivial transverse scalar field z := x 6 with the profile σ denotes the radial distance in the directions (2345) transverse to the self-dual string along the fivebrane worldvolume. Q sd is the electric (equally magnetic) charge of the self-dual string.
(2) As a three-funnel solution of the Basu-Harvey equation [3], which has been proposed as an M-theoretic generalization of the Nahm equations for the BIon. This is an alternative M2-based description of (1) that refers again to the case of a single M5 brane.
(3) As a 1/4-BPS supergravity solution in the regime of a large number of M2 and M5 branes. There has been considerable work in this direction (see [4][5][6] for earlier studies).
A fully localized intersection was described in [7], where the solution is given in terms of two functions that obey a set of differential equations.
In what follows we will describe the M2-M5 intersection from the supergravity perspective (3) using the blackfold formalism [8][9][10]. This is an effective worldvolume description of black brane dynamics which is part of a perturbative expansion scheme of the gravitational equations and belongs conceptually to the same class of ideas as the fluid-gravity correspondence for AdS black branes [11,12]. In the present case we will be interested in the effective fivebrane worldvolume dynamics of the M2-M5 bound state [13][14][15][16][17]. We will restrict our attention to the leading order form of this effective description assuming small accelerations in a derivative expansion in a manner very similar in spirit to the zero-th order approximation typically employed in applications of the Dirac-Born-Infeld action for standard D-branes in string theory. As in the case of the BIon solution for the F1-D3 system [18], we will see that the zero-th order solution can take us far enough.
Although a perturbative reconstruction of the exact supergravity solution is in principle possible in this manner, working with an effective worldvolume description -as we will do here-has some obvious benefits. We should note that a similar treatment of the BIon solution for the F1-D3 system was given recently in two beautiful papers [19,20]. The F1-D3 intersection is U-dual to the M2-M5 system (1.1) and inevitably the application of the blackfold formalism in [19,20] shares several common features with the application in this note. 1 Our goal is to highlight those features that are particularly interesting from an M-theory perspective and contrast them with the results in the existing literature as a basis for further work in this direction.
The basics of the blackfold approach and the elements we need for the present application are summarized in section 2. Section 3 presents the main results of this paper, which include the self-dual string soliton solution and the key properties of related wormhole solutions. A more detailed and more general treatment of the system will be given in a companion paper [21]. A brief discussion of the results and future directions appears in the concluding section 4.
1 Recall, however, that the direct application of U-dualities in supergravity typically does not produce fully localized intersections. Regarding the specific relation between the F1-D3 and M2-M5 systems this point is also noted, and properly taken into account, in [7].

Planar M2-M5 bound state
Our starting point is a well-known exact solution of the eleven dimensional supergravity equations of motion that describes the black M2-M5 bound state [13][14][15][16][17] 2) 3) C 3 is the standard three-form potential of the 11d supergravity action and C 6 its Hodgedual. The solution, which describes M2 brane charge dissolved into the worldvolume of the black fivebrane along the (012) plane, is parameterized by the constants r 0 , α and θ which control the temperature, the M2 and the M5 brane charge.
We will reserve the notation Q for charges and Q for charge densities. In this notation A corresponding free energy F can be defined as where Ω (n) denotes the volume of the round n-sphere.
Under the general boost along the fivebrane worldvolume directions the stress-energy tensor of the above solution takes the form ab , a, b, ... = 0, 1, . . . , 5 (2.7) where, following closely the notation of [10], u a denotes a unit 6-velocity field, η ab the flat induced worldvolume metric, and h (q) ab (q = 2, 5) is a projector along the worldvolume directions of the M2 and M5 branes respectively. In the case of (2.1)-(2.4) h (2) ab projects along the plane (012) and h (5) ab = η ab .

Leading order blackfold equations
One can use the planar solution (2.1)-(2.4) as the zero-th order term in a perturbative expansion to construct more complicated solutions with inhomogeneous, spinning, and bending worldvolume geometries. The effective degrees of freedom in such a longwavelength description are the parameters r 0 , α, θ, and the velocities u a that characterize the zero-th order solution, five transverse scalars that capture the bending of the M5 in its eleven dimensional ambient space, and a unit three-form that captures the local M2 brane current and its distribution within the larger fivebrane worldvolume. The self-dual three-form field strength of the M5 brane has disappeared in this regime and has been replaced by corresponding conserved currents.
In analogy to usual practice in the fluid-gravity correspondence for AdS black branes, one promotes the above parameters to slowly varying functions of the local worldvolume coordinates σ a (a = 0, 1, . . . , 5) and proceeds to solve the gravitational equations perturbatively in a derivative expansion. A subset of the gravity equations are constraint equations. Satisfying them at a given order n is believed to guarantee the existence of a regular solution up to the (n + 1)-th order in the expansion scheme (see [22] for a recent derivation of this statement for n = 0 in pure Einstein gravity and [23,24] for a discussion of higher derivative corrections). This is the general framework of the blackfold formalism. In what follows we will restrict our attention to the leading order constraint equations which are believed to guarantee the existence of a regular supergravity solution up to the next-to-leading order in the expansion. In our case these equations can be formulated as follows (for more details we refer the reader to [9,25,10]).

Intrinsic equations.
They comprise of the fluid-dynamical equations D a T ab = 0 (2.8) and the charge conservation equations for the M2 and M5 brane currents respectively. The latter trivially leads to In these equations the stress-energy tensor (2.7) is promoted to where γ ab is now the general induced worldvolume metric.V (3) denotes a unit volume 3-form along the directions of the M2 brane current andV (6) the unit volume form of the fivebrane worldvolume. The last equation (2.11) shows that Q 5 is an overall constant that participates passively into the dynamics. The M2 brane charge density and its distribution inside the fivebrane worldvolume, however, are dynamical quantities controlled by (2.8), (2.9).

Extrinsic equations.
These comprise of the remaining set of the stress-energy conservation equations and can be recast into the form or equivalently in a more detailed form as (2.14) K ab ρ is the extrinsic curvature tensor [9], K ρ the mean curvature vector, ⊥ ρ µ a projector in directions orthogonal to the fivebrane worldvolume and In the following section we are looking for simple static solutions of the above equations.

Static ansatz
In what follows we will concentrate on a rather restricted simple class of static S 3funnel solutions that extend the self-dual string soliton of Ref.
[2] to our context. More general solutions are possible and will be discussed in a companion paper along with a more detailed exposition of the relevant steps.
We will make use of the following parametrization of the ambient eleven dimensional flat spacetime using the standard angular coordinates (ψ, ϕ, ω) to express the round three-sphere metric We choose the static gauge activating only one of the transverse scalars x 6 := z(σ) in accordance with (1.1). With this ansatz the induced metric on the effective fivebrane worldvolume is By setting and by demanding that the quantities q 2 , q 5 , β, defined as

7)
r 0 coshα = β := 3 4πT (3.8) are constants of motion independent of σ a , one can show that the intrinsic equations (2.8), (2.9), (2.11) are fully satisfied. In these relations Q 2 and Q 5 are the total M2 and M5 brane charges, expressed in terms of the number of M2 and M5 branes (N 2 , N 5 ) as (3.9) T is the global constant temperature of the solution and ℓ P the Planck scale (in terms of which 16πG = (2π) 8 ℓ 9 P ). These expressions allow us to determine completely the dynamics of the unknown functions r 0 , α, θ. After a minor algebraic computation one finds two solutions (both acceptable) with We are using the convenient definition It is also worth noting that the first expression (3.10) implies an upper bound on the temperature T β 3 ≥ 2|q 5 | . (3.14) The final step requires solving the extrinsic equations (2.13). Inserting the solutions (3.10)-(3.12) into (2.13) we obtain equations of motion exclusively for the transverse scalars.
It has been shown [9,25,10] on general grounds for stationary configurations that these equations can also be obtained from the variation of the action functional where F is the free energy (2.6) viewed as a functional of the transverse scalars, and the variation with respect to the transverse scalars is performed keeping the temperature and corresponding charges fixed. W 6 is the six dimensional fivebrane worldvolume. In the case at hand the action (3.15) becomes L t , L x 1 denote the (infinite) length of the t, x 1 directions. We conclude that the corresponding equation of motion for the transverse scalar field z(σ) is The prime denotes differentiation with respect to σ.
In analogy to the BIon case [18,19] we will find spike and wormhole solutions to this equation representing M2 branes ending on M5 branes or M2 branes stretching between M5 and anti-M5 branes. The leading order approximation is valid as long as the following condition is met [19,21] σ ≫ r c (σ) , r 3 c = r 3 0 sinhα coshα , (3.19) where r c is the charge radius of the black brane [25,10]. Nevertheless, as in the DBI case [18], and especially in extremal situations, the naive extrapolation of the leading order result beyond this regime continues to give qualitatively and quantitatively sensible results.

1/4-BPS spike
Only the + branch in (3.16), (3.17) has a sensible extremal limit. In this limit, where T → 0 and β → +∞, the action (3.16) simplifies to The validity of approximation (3.19) breaks down when where we made use of (3.7),(3.12). Irrespective of this breakdown, we observe that the leading order solution is well-defined for all σ ∈ IR + and, as we will see in a moment, the reproducing correctly the tension of N 2 BPS M2 branes. T M 2 denotes the tension of a single M2 brane.
In addition, the transverse scalar profile N 5 in our case. This seems to imply that the effective transverse scalar degree of freedom of the blackfold description is an average over the M5 branes, which is presumably a sign of the importance of abelian dynamics in the supersymmetric non-thermal case. A similar situation is encountered in supertubes [26]. It would be useful to obtain a better understanding of the more general (holographic) relation between the blackfold effective degrees of freedom and the microscopic degrees of freedom of the multiple M5 brane theory. 2 Regardless of the specifics of this relation it is interesting to note the direct analogies between the way the known non-gravitational M5 brane worldvolume description works and how the blackfold description repackages the information of the gravitational solutions. This is one of the conceptual advantages of the blackfold approach.

Thermal spikes
By adding temperature to the above configuration the corresponding black brane intersection becomes non-extremal. Following the general discussion of subsection 3.1 we are now looking for a spike solution of the + branch equation (3.18) at finite β. However, unlike the zero-temperature case such a solution does not exist over the full range of σ, i.e. for σ ∈ IR + . The failure to obtain a sensible solution below a certain value of σ is immediately obvious from eqs. (3.10), (3.11). For finite β, as we decrease σ we reach a critical breakdown value, σ b , where the term under one of the square roots becomes zero and then negative. This critical value equals The inequality (3.14) guarantees that the denominator in this expression is non-negative.
From the small temperature expansion of (3.25) at fixed q 2 , q 5 , (3.26) and the expression for the critical point of breakdown of the validity of the approximation for the extremal spike (3.23) we deduce that up to leading order in temperature Hence, the breakdown of the leading order thermal spike solution occurs (at least within the small temperature expansion) well within the region where the leading order blackfold approximation cannot be trusted. In that sense, the pathological region is automatically excised and poses no particular concern. The only issue we have to worry about is the issue of boundary conditions. Which one of the solutions of the differential equation (3.18) does one pick for a given temperature? We will discuss the more general solutions of the differential equation (3.18) in the following subsection.
The same issue was encountered for thermal spikes of the F1-D3 system in [20]. The strategy adopted in that paper was based on finding a matching point where an F1-D3 thermal spike solution could be glued to a non-extremal black F-string at the desired temperature. More precisely, the thermal spike solution was chosen to reproduce the tension of a non-extremal black F-string.
An analogous approach can be taken in our case. We can fix the solution of the differential equation (3.18) by matching the tension of a planar black M2 brane to the local tension of the thermal spike at a suitably chosen temperature-dependent σ 0 . Since many of the details go in complete analogy with the BIon case of [20] we will not discuss them further in this note. The resulting solution describes a thermalized self-dual string soliton solution.

Wormhole solutions
The most general solution of the differential equation (3.18) with the boundary con- is parametrized by a value σ 0 , which is defined so that Integrating the differential equation (3.18) with these boundary conditions we find In this form the solution extends over the range σ ∈ [σ 0 , +∞) and one has to decide how to extend it beyond this domain. In the previous subsection we considered the possibility of gluing a planar black M2 brane. Another possibility is to glue back at σ 0 the same solution with the opposite orientation. The resulting configuration describes a bi-funnel, or wormhole-like solution that stretches between a stack of M5 and anti-M5 branes. Analogous configurations for the BIon were considered in [18,19]. A configuration at non-zero σ 0 can be extremal but not BPS.
In what follows we summarize some of the main features of the wormhole solutions.
It will be convenient to define the distance between the M5 and anti-M5 stacks as where F = F ± . Notice the scaling property ∆(σ 0 ; T, κ) = κ ; T, 1 .

Extremal wormholes
Once again, only the + branch is relevant for the extremal limit. The solution has an analytic form for any σ 0 The corresponding distance ∆ reads Its behavior as a function of σ 0 is depicted in Fig. 1. Analogous wormhole solutions can be found in the case of a single M5 brane using the fivebrane worldvolume theory [27][28][29] or by uplifting to M-theory the BIon solutions of [18].
We observe that there is a minimum distance between the two fivebranes that occurs for σ 0,min = 2

Branch connected to extremal wormholes
For the + branch and finite β the distance ∆ is given by the expression (3.32) with F = F + . We have not been able to find a closed analytic expression for generic values of the temperature. The small temperature expansion takes the form where ∆ 0 is the extremal result (3.35) and Accordingly, the minimum we observed before is shifted to σ 0,min = 2  Analogous features have been observed for the thermal BIon solution [20].

Wormholes of the neutral branch
The solution based on the F − function connects naturally to the neutral black fivebrane solution. This can be seen in the following manner.
In the low temperature limit the corresponding solution has the expansion z(σ) = 1 + In this paper we have applied this formalism to the basic M2-M5 intersection extending previous work on the F1-D3 system [19,20]. Our main purpose has been to demonstrate how the formalism works in a simple representative situation and to relate the basic results with previous standard results in the literature of the M2-M5 system. In particular, we have seen (i) how one recovers the 1/4-BPS self-dual string soliton solution extending the single M5 brane result of [2] to the regime of many M2 and M5 branes, and (ii) how one can access the properties of the self-dual string soliton at finite temperature. The discussion of the supersymmetric self-dual string soliton is directly related to the exact supergravity analysis of [7]. The non-extremal configurations in this paper provide, to the best of our knowledge, the first information for this type of black brane intersections in eleven dimensional supergravity.
The approach can be used to further probe the M2-M5 system in more generic situations. In a companion paper [21] we discuss M2-M5 intersections at finite temperature and angular momentum. We present the corresponding solutions and compute their thermodynamic properties.
In this note we have focused on the M2-M5 system in flat space. It is equally possible to discuss it in other backgrounds, for instance in AdS and within the context of the AdS/CFT correspondence. Analogous discussions in AdS using the worldvolume description of a single M5 brane have appeared in [30][31][32]. Blackfolds in AdS have been analyzed in the past in [33][34][35].
Perhaps the most pressing question is whether we can use the approach presented in this work to obtain new information about some of the currently inaccessible properties of the self-dual string soliton (and corresponding properties of the M5 brane). The fact that we can access the system in the regime of many M5 branes (which lies beyond the reach of most other methods) is encouraging. Since we work in the supergravity regime with an effective field theory tool the relation with the still illusive microscopic description of the M5 theory is indirect, however, it is not unreasonable to expect that the information obtained with our approach can provide new useful clues about the microscopic structure.
Work in this direction is currently underway.