The relationship between modern physics and knot physics.
In this paper, the Kelvin wave and knot dynamics are studied on three dimensional smoothly deformed entangled vortex-membranes in five dimensional space. Owing to the existence of local Lorentz invariance and diffeomorphism invariance, in continuum limit gravity becomes an emergent phenomenon on 3 + 1 dimensional zero-lattice (a lattice of projected zeroes): on the one hand, the deformed zero-lattice can be denoted by curved space-time for knots; on the other hand, the knots as topological defect of 3 + 1 dimensional zero-lattice indicates matter may curve space-time. This work would help researchers to understand the mystery in gravity.
A vortex (point-vortex, vortex-line, vortex-membrane) consists of the rotating motion of fluid around a common centerline. It is defined by the vorticity in the fluid, which measures the rate of local fluid rotation. In three dimensional (3D) superfluid (SF), the quantization of the vorticity manifests itself in the quantized circulation where is Planck constant and is atom mass of SF. Vortex-lines can twist around its equilibrium position (common centerline) forming a transverse and circularly polarized wave (Kelvin wave) [1, 2]. Because Kelvin waves are relevant to Kolmogorov-like turbulence [3, 4], a variety of approaches have been used to study this phenomenon. For two vortex-lines, owing to the interaction, the leapfrogging motion has been predicted in classical fluids from the works of Helmholtz and Kelvin [5, 6, 7, 8, 9, 10]. Another interesting issue is entanglement between two vortex-lines. In mathematics, vortex-line-entanglement can be characterized by knots with different linking numbers. The study of knotted vortex-lines and their dynamics has attracted scientists from diverse settings, including classical fluid dynamics and superfluid dynamics [11, 12].
In the paper , the Kelvin wave and knot dynamics in high dimensional vortex-membranes were studied, including the leapfrogging motion and the entanglement between two vortex-membranes. A new theory—
In this paper, we will study the Kelvin wave and knot dynamics on 3D deformed knot-crystal, particularly the topological interplay between knots and the lattice of projected zeroes (we call it zero-lattice). Owing to the existence of local Lorentz invariance and diffeomorphism invariance, the gravitational interaction emerges: on the one hand, the deformed zero-lattice can be denoted by curved space-time; on the other hand, the knots deform the zero-lattice that indicates matter may curve space-time (see below discussion).
The paper is organized as below. In Section 2, we introduce the concept of “zero-lattice” from projecting a knot-crystal. In addition, to characterize the entangled vortex-membranes, we introduce geometric space and winding space. In Section 3, we derive the massive Dirac model in the vortex-representation of knot states on geometric space and that on winding space. In Section 4, we consider the deformed knot-crystal as a background and map the problem onto Dirac fermions on a curved space-time. In Section 5, the gravity in knot physics emerges as a topological interplay between zero-lattice and knots and the knot dynamics on deformed knot-crystal is described by Einstein’s general relativity. Finally, the conclusions are drawn in Section 6.
2. Knot-crystal and the corresponding zero-lattice
Knot-crystal is a system of two periodically entangled vortex-membranes that is described by a special pure state of Kelvin waves with fixed wave length [13, 14]. In emergent quantum mechanics, we consider knot-crystal as a ground state for excited knot states, i.e.,
On the one hand, a knot is a piece of knot-crystal and becomes a topological excitation on it; on the other hand, a knot-crystal can be regarded as a composite system with multi-knot, each of which is described by same tensor state.
Because a knot-crystal is a plane Kelvin wave with fixed wave vector , we can use the tensor representation to characterize knot-crystals ,
where and , are Pauli matrices for helical and vortex degrees of freedom, respectively. For example, a particular knot-crystal is called SOC knot-crystal , of which the tensor state is given by
For the SOC knot-crystal, along
For a knot-crystal, another important property is generalized spatial translation symmetry that is defined by the translation operation
Here is . For example, for the knot states on 3D SOC knot-crystal, the translation operation along -direction becomes
2.2. Winding space and geometric space
For a knot-crystal, we can study it properties on a 3D space (). In the following part, we call the space of ()
For a 1D leapfrogging knot-crystal that describes two entangled vortex-lines with leapfrogging motion, the function is given by
where is angular frequency of leapfrogging motion. For the 1D -knot-crystal, the coordinate on winding space is . Another example is 3D SOC knot-crystal , of which the function is given by
where the coordinates on winding space are , , , respectively.
In addition, there exists generalized spatial translation symmetry on winding space. On winding space, the translation operation becomes
where denotes the distance on winding space.
Before introduce zero-lattice, we firstly review the projection between two entangled vortex-membranes along a given direction in 5D space by
where is variable and is constant. So the projected vortex-membrane is described by the function . For two projected vortex-membranes described by and , a zero is solution of the equation
After projection, the knot-crystal becomes a zero lattice. For example, a 1D leapfrogging knot-crystal is described by
According to the knot-equation , we have
where and is the position of zero. As a result, we have a periodic distribution of zeroes (knots).
For a 3D leapfrogging SOC knot-crystal described by , we have similar situation—the solution of zeroes does not change when the tensor order changes, i.e., with . We call the periodic distribution of zeroes to be
Along a given direction , after shifting the distance , the phase angle of vortex-membranes in knot-crystal changes , i.e.,
Thus, on the winding space, we have a corresponding “zero-lattice” of discrete lattice sites described by the three integer numbers
3. Dirac model for knot on zero-lattice
3.1. Dirac model on geometric space
3.1.1. Dirac model in sublattice-representation on geometric space
It was known that in emergent quantum mechanics, a 3D SOC knot-crystal becomes multi-knot system, of which the effective theory becomes a Dirac model in quantum field theory. In emergent quantum mechanics, the Hamiltonian for a 3D SOC knot-crystal has two terms—the kinetic term from global winding and the mass term from leapfrogging motion. Based on a representation of projected state, a 3D SOC knot-crystal is reduced into a “two-sublattice” model with discrete spatial translation symmetry, of which the knot states are described by and (or the Wannier states and ). We call it the Dirac model in
In sublattice-representation on geometric space, the equation of motion of knots is determined by the Schrödinger equation with the Hamiltonian
where is an four-component fermion field as . Here, label two chiral-degrees of freedom that denote the two possible sub-lattices, label two spin degrees of freedom that denote the two possible winding directions. We have
is the momentum operator. plays role of the mass of knots and play the role of light speed where is a fixed length that denotes the half pitch of the windings on the knot-crystal.
In addition, the low energy effective Lagrangian of knots on 3D SOC knot-crystal is obtained as
where , are the reduced Gamma matrices,
3.1.2. Dirac model in vortex-representation on geometric space
In this paper, we derive the effective Dirac model for a knot-crystal based on a representation of vortex degrees of freedom. We call it
In Ref. , it was known that a knot has four degrees of freedom, two spin degrees of freedom or from the helicity degrees of freedom, the other two vortex degrees of freedom from the vortex degrees of freedom that characterize the vortex-membranes, or . The basis to define the microscopic structure of a knot is given by , , , .
We define operator of knot states by the region of the phase angle of a knot: for the case of , we have ; for the case of , we have . As shown in Figure 2 , we label the knots by Wannier state , , , ….
To characterize the energy cost from global winding, we use an effective Hamiltonian to describe the coupling between two-knot states along -direction on 3D SOC knot-crystal
with the annihilation operator of knots at the site , . is the coupling constant between two nearest-neighbor knots. According to the generalized translation symmetry, the transfer matrices along -direction are defined by
After considering the spin rotation symmetry and the symmetry of vortex-membrane-A and vortex-membrane-B, the effective Hamiltonian from global winding energy can be described by a familiar formulation
We then use path-integral formulation to characterize the effective Hamiltonian for a knot-crystal as
where and . To describe the knot states on 3D knot-crystal, we have introduced a four-component fermion field to be
where label vortex degrees of freedom and label two spin degrees of freedom that denote the two possible winding directions along a given direction .
In continuum limit, we have
where the dispersion of knots is
where and is the velocity. In the following part we ignore .
Next, we consider the mass term from leapfrogging motion, of which the angular frequency . For leapfrogging motion obtained by , the function of the two entangled vortex-membranes at a given point in geometric space is simplified by
At , we have ; at , we have . The leapfrogging knot-crystal leads to periodic varied knot states, i.e., at we have a knot on vortex-membrane-A that is denoted by ; at we have a knot on vortex-membrane-B denoted by . As a result, the leapfrogging motion becomes a global winding along time direction, , , , , … See the illustration of vortex-representation of knot states for knot-crystal in Figure 2(c) . After a time period , a knot state turns into a knot state . Thus, we use the following formulation to characterize the leapfrogging process,
After considering the energy from the leapfrogging process, a corresponding term is given by
From the global rotating motion denoted , the winding states also change periodically. Because the contribution from global rotating motion is always canceled by shifting the chemical potential, we do not consider its effect.
From above equation, in the limit we derive low energy effective Hamiltonian as
We then re-write the effective Hamiltonian to be
is the momentum operator. is the annihilation operator of four-component fermions. plays role of the mass of knots and play the role of light speed where is a fixed length that denotes the half pitch of the windings on the knot-crystal. In the following parts, we set and .
Due to Lorentz invariance (see below discussion), the geometric space becomes geometric space-time, i.e., . Here, we may consider and to be
Finally, the low energy effective Lagrangian of 3D SOC knot-crystal is obtained as
where , are the reduced Gamma matrices,
In addition, we point out that there exists intrinsic relationship between the knot states of sublattice-representation and the knot states of vortex-representation
where . From the sublattice-representation of knot states, the knot-crystal becomes an object with staggered R/L zeroes along
3.1.3. Emergent Lorentz-invariance
We discuss the emergent Lorentz-invariance for knot states on a knot-crystal.
Since the Fermi-velocity only depends on the microscopic parameter and , we may regard to be “light-velocity” and the invariance of light-velocity becomes an fundamental principle for the knot physics. The Lagrangian for massive Dirac fermions indicates emergent SO(3,1) Lorentz-invariance. The SO(3,1) Lorentz transformations is defined by
For a knot state with a global velocity , due to SO(3,1) Lorentz-invariance, we can do Lorentz boosting on by considering the velocity of a knot,
We can do non-uniform Lorentz transformation on knot states . The
For a particle-like knot, a uniform wave-function of knot states is
Under Lorentz transformation with small velocity , this wave-function is transformed into
where , and . As a result, we derive a new distribution of knot-pieces by doing Lorentz transformation, that are described by the plane-wave wave-function . The new wave-function comes from the Lorentz boosting .
Noninertial system can be obtained by considering non-uniformly velocities, i.e., . According to the linear dispersion for knots, we can do local Lorentz transformation on i.e.,
We can also do non-uniform Lorentz transformation on knot states , i.e.,
where the new wave-functions of all quantum states change following the non-uniform Lorentz transformation . It is obvious that there exists intrinsic relationship between noninertial system and curved space-time.
3.2. Dirac model on winding space
In this part, we show the effective Dirac model of knot states on winding space.
The coordinate measurement of zero-lattice on winding space is the winding angles, . Along a given direction , after shifting the distance , the winding angle changes . The position is determined by two kinds of values: are integer numbers
and denote internal winding angles
Therefore, on winding space, the effective Hamiltonian turns into
where and . Because of , quantum number of is angular momentum and the energy spectra are . If we focus on the low energy physics (or ), we may get the low energy effective Hamiltonian as
For low energy physics, the position in 3 + 1D winding space-time is 3 + 1D zero-lattice of winding space-time labeled by four integer numbers, where
The lattice constant of the winding space-time is always that will never be changed. As a result, the winding space-time becomes an effective
4. Deformed zero-lattice as curved space-time
In this section, we discuss the knot dynamics on smoothly deformed knot-crystal (or deformed zero-lattice). We point out that to characterize the entanglement evolution, the corresponding Biot-Savart mechanics for a knot on smoothly deformed zero-lattice is mapped to that in quantum mechanics on a curved space-time.
4.1. Entanglement transformation
Firstly, based on a uniform 3D knot-crystal (uniform entangled vortex-membranes), we introduce the concept of “
Under global entanglement transformation, we have
Here, and are constant winding angles along spatial -direction and that along tempo direction on geometric space-time, respectively. The dispersion of the excitation changes under global entanglement transformation.
In general, we may define (local) entanglement transformation, i.e.,
where and are not constant. We call a system with smoothly varied-(, )
4.2. Geometric description for deformed zero-lattice: curved space-time
For knots on a deformed zero-lattice, there exists an intrinsic correspondence between an entanglement transformation and a local coordinate transformation that becomes a fundamental principle for emergent gravity theory in knot physics.
For zero-lattice, changes the winding degrees of freedom that is denoted by the local coordination transformation, i.e.,
These equations also imply a curved space-time: the lattice constants of the 3 + 1D zero-lattice (the size of a lattice constant with angle changing) are not fixed to be , i.e.,
The distance between two nearest-neighbor “lattice sites” on the spatial/tempo coordinate changes, i.e.,
where and are the unit-vectors of the original frame and the deformed frame, respectively. See the illustration of a 1 + 1D deformed zero-lattice on winding space-time with a non-uniform distribution of zeroes in Figure 3(d) .
However, for deformed zero-lattice, the information of knots in projected space is invariant: when the lattice-distance of zero-lattice changes , the size of the knots correspondingly changes . Therefore, due to the invariance of a knot, the deformation of zero-lattice does not change the formula of the low energy effective model for knots on winding space-time. Because one may smoothly deform the zero-lattice and get the same low energy effective model for knots on winding space-time, there exists
Therefore, from the view of mathematics, the physics on winding space-time is never changed! The invariance of the effective model for knots on winding space-time indicates the diffeomorphism invariance
On the other hand, the condition of very smoothly entanglement transformation guarantees a (
According to the local coordinate transformation, the deformed zero-lattice becomes a curved space-time for the knots. In continuum limit and , the diffeomorphism invariance and (local) Lorentz invariance emerge together. E. Witten had made a strong claim about emergent gravity, “
To characterize the deformed 3 + 1D zero-lattice , we introduce a geometric description. In addition to the existence of a set of vierbein fields , the space metric is defined by where is the internal space metric tensor. The geometry fields (vierbein fields and spin connections ) are determined by the non-uniform local coordinates . Furthermore, one needs to introduce spin connections and the Riemann curvature two-form as
where are the components of the usual Riemann tensor projection on the tangent space. The deformation of the zero-lattice is characterized by
So the low energy physics for knots on the deformed zero-lattice turns into that for Dirac fermions on curved space-time
where and . This model described by is invariant under local (non-compact) SO(3,1) Lorentz transformation as
is invariant under local SO(3,1) Lorentz symmetry as
In general, an SO(3,1) Lorentz transformation is a combination of spin rotation transformation and Lorentz boosting .
In physics, under a Lorentz transformation, a distribution of knot-pieces changes into another distribution of knot-pieces. For this reason, the velocity and the total number of zeroes are invariant,
4.3. Gauge description for deformed zero-lattice
4.3.1. Deformed entanglement matrices and deformed entanglement pattern
The deformation of the zero-lattice leads to deformation of entanglement pattern, i.e.,
denotes the space-time position of a site of zero-lattice, . Each entanglement matrix becomes a unit SO(4) vector-field on each lattice site. The deformed zero-lattice induced by local entanglement transformation is characterized by four SO(4) vector-fields (four entanglement matrices) . See the illustration of a 2D deformed zero-lattice in Figure 4(d) , in which the arrows denote deformed entanglement matrix .
4.3.2. Gauge description for deformed tempo entanglement matrix
Firstly, we study the unit SO(4) vector-field of deformed tempo entanglement matrix . To characterize , the reduced Gamma matrices is defined as
Under this definition (), the effect of deformed zero-lattice from spatial entanglement transformation , , can be studied due to
However, the effect of deformed zero-lattice from tempo entanglement transformation cannot be well defined due to
We introduce an SO(4) transformation that is a combination of spin rotation transformation and spatial entanglement transformation (entanglement transformation along
Here, denotes operation combination. Under a non-uniform SO(4) transformation , we have
where is a unit SO(4) vector-field. For the deformed zero-lattice, according to , the entanglement matrix along tempo direction is varied, .
In general, the SO(4) transformation is defined by . Under the SO(4) transformation, we have
In particular, is invariant under the SO(4) transformation as
The correspondence between index of and index of space-time is
We denote this correspondence to be
where denotes the index order of and denotes the index order of space-time .
As a result, we can introduce an auxiliary gauge field and use a gauge description to characterize the deformation of the zero-lattice. The auxiliary gauge field is written into two parts : SO(3) parts
and SO(4)/SO(3) parts
The total field strength of components can be divided into two parts
According to pure gauge condition, we have Maurer-Cartan equation,
Finally, we emphasize the equivalence between and , i.e., .
4.3.3. Gauge description for deformed spatial entanglement matrix
Next, we study the unit SO(4) vector-field of deformed spatial entanglement matrix . To characterize , the reduced Gamma matrices is defined as
Here, , , and are three orthotropic spatial entanglement matrices. Under this definition (), the effect of deformed zero-lattice from partial spatial/tempo entanglement transformation , , can be studied due to
However, the effect of deformed zero-lattice from spatial entanglement transformation cannot be well defined due to
We use similar approach to introduce the gauge description. We can also define the reduced Gamma matrices as
The correspondence between index of and index of space-time is
We denote this correspondence to be
Now, the SO(4) transformation is not a combination of spin rotation symmetry and entanglement transformation along
where is a unit vector-field. The auxiliary gauge field are defined by
According to pure gauge condition, we also have the following Maurer-Cartan equation,
Finally, we emphasize the equivalence between and , i.e., , , .
4.3.4. Hidden SO(4) invariant for gauge description
In addition, there exists a hidden global SO(4) invariant for entanglement matrices along different directions in 3 + 1D (winding) space-time . To show the hidden SO(4) invariant, we define the reduced Gamma matrices as
with . Here, , , , are constant.
Under this description, we can study the entanglement deformation along orthotropic spatial/tempo directions to .
4.4. Relationship between geometric description and gauge description for deformed zero-lattice
Due to the generalized spatial translation symmetry there exists an
On the one hand, to characterize the changes of the positions of zeroes, we must consider a curved space-time by using geometric description, . On the other hand, we need to consider a varied vector-field
by using gauge description. There exists intrinsic relationship between the geometry fields and the auxiliary gauge fields .
For a non-uniform zero-lattice, we have
On deformed zero-lattice, the “lattice distances” become dynamic vector fields. We define the vierbein fields that are supposed to transform homogeneously under the local symmetry, and to behave as ordinary vectors under local entanglement transformation along -direction,
For the smoothly deformed vector-fields , within the representation of we have
Thus, the relationship between and is obtained as
According to this relationship, the changing of entanglement of the vortex-membranes curves the 3D space.
On the other hand, within the representation of we have
According to this relationship, the changing of entanglement of the vortex-membranes curves the 4D space-time.
In addition, we point out that for different representation of reduced Gamma matrix, there exists intrinsic relationships between the gauge fields and . After considering these relationships, we have a complete description of the deformed zero-lattice on the geometric space-time,
5. Emergent gravity
Gravity is a natural phenomenon by which all objects attract one another including galaxies, stars, human-being and even elementary particles. Hundreds of years ago, Newton discovered the inverse-square law of universal gravitation, where is the Newton constant, is the distance, and and are the masses for two objects. One hundred years ago, the establishment of general relativity by Einstein is a milestone to learn the underlying physics of gravity that provides a unified description of gravity as a geometric property of space-time. From Einstein’s equations , the gravitational force is really an effect of curved space-time. Here is the 2nd rank Ricci tensor, is the curvature scalar, is the metric tensor, and is the energy-momentum tensor of matter.
In this section, we point out that there exists emergent gravity for knots on zero-lattice.
5.1. Knots as topological defects
5.1.1. Knot as SO(4)/SO(3) topological defect in 3 + 1D space-time
A knot corresponds to an elementary object of a knot-crystal; a knot-crystal can be regarded as composite system of multi-knot. For example, for 1D knot, people divide the knot-crystal into identical pieces, each of which is just a knot.
From point view of
From point view of
As a result, a knot looks like a special type of edge dislocation on 3 + 1D zero-lattice. The zero-lattice is deformed and becomes mismatch with an additional knot.
From point view of
In mathematics, to generate a knot at , we do global topological operation on the knot-crystal, i.e.,
with and ;
with and ;
with and ;
with and . As a result, due to the rotation symmetry in 3 + 1D space-time, a knot becomes SO(4)/SO(3) topological defect. Along arbitrary direction, the local entanglement matrices around a knot at center are switched on the tangential sub-space-time.
5.1.2. Knot as SO(3)/SO(2) magnetic monopole in 3D space
To characterize the topological property of a knot on the 3 + 1D zero-lattice, we use gauge description. We firstly study the tempo entanglement deformation and define . Under this gauge description, we can only study the effect of a knot on three spatial zero-lattice.
When there exists a knot, the periodic boundary condition of knot states along arbitrary direction is changed into anti-periodic boundary condition,
Consequently, along given direction (for example -direction), the local entanglement matrices on the tangential sub-space are switched by . Along -direction, in the limit of , we have the local entanglement matrices on the tangential sub-space as and ; in the limit of , we have the local entanglement matrices on the tangential sub-space as and .
Because we have similar result along -direction for the system with an extra knot, the system has generalized spatial rotation symmetry. Due to the generalized spatial rotation symmetry, when moving around the knot, the local tangential entanglement matrices (we may use indices , to denote the sub space) must rotate synchronously. See the red arrows that denote local tangential entanglement matrices in Figure 4(c) and (d) . In Figure 4(d) , local tangential entanglement matrices induced by an extra (unified) knot shows vortex-like topological configuration in projected 2D space (for example,
To characterize the topological property of 3 + 1D zero-lattice with an extra (unified) knot, we apply gauge description and write down the following constraint
and . The upper indices of label the local entanglement matrices on the tangential sub-space and the lower indices of denote the spatial direction. The non-zero Gaussian integrate just indicates the local entanglement matrices on the tangential sub-space to be the local frame of an orientable sphere with fixed chirality.
As a result, the entanglement pattern with an extra 3D knot is topologically deformed and the 3D knot becomes SO(3)/SO(2)
where is the “magnetic” charge of auxiliary gauge field . For single knot , the “magnetic” charge is .
5.1.3. Knot as SO(3)/SO(2) magnetic monopole in 2 + 1D space-time
Next, we study the spatial entanglement deformation and define . Under this gauge description, we can only study the effect of a knot on 2D spatial zero-lattice and 1D tempo zero-lattice.
In the 2 + 1D space-time, a knot also leads to -phase changing,
Due to the spatial-tempo rotation symmetry, the knot also becomes SO(3)/SO(2) magnetic monopole and traps a “magnetic charge” of the auxiliary gauge field , i.e.,
where is the “magnetic” charge of auxiliary gauge field . Remember that the correspondence between index of and index of space-time is , , .
To characterize the induced magnetic charge, we write down another constraint
The upper indices of denote the local entanglement matrices on the tangential sub-space-time and the lower indices of denote the spatial direction. Therefore, according to above equation, the 2 + 1D zero-lattice is globally deformed by an extra knot.
In general, due to the hidden SO(4) invariant, for other gauge descriptions , a knot also play the role of SO(3)/SO(2) magnetic monopole and traps a “magnetic charge” of the corresponding auxiliary gauge field.
5.2. Einstein-Hilbert action as topological mutual BF term for knots
It is known that for a given gauge description, a knot is an SO(3)/SO(2) magnetic monopole and traps a “magnetic charge” of the corresponding auxiliary gauge field. For a complete basis of entanglement pattern, we must use four orthotropic SO(4) rotors and four different gauge descriptions to characterize the deformation of a knot (an SO(4)/SO(3) topological defect) on a 3 + 1D zero-lattice.
Firstly, we use Lagrangian approach to characterize the deformation of a knot (an SO(3)/SO(2) topological defect) on a 3D spatial zero-lattice, . The topological constraint in Eq. (117) can be re-written into
where is covariant derivative in 3 + 1D space-time. is a field that plays the role of Lagrangian multiplier. The upper index of denotes the local radial entanglement matrix around a knot, along which the entanglement matrix does not change. Thus, we use the dual field to enforce the topological constraint in Eq. (117). That is, to denote the upper index of that is the local tangential entanglement matrices, we set antisymmetric property of upper index of and that of . Because and have the same SO(3,1) generator , due to SO(3,1) Lorentz invariance we can do Lorentz transformation and absorb the dual field into , i.e., . As a result, the dual field is replaced by .
In the path-integral formulation, to enforce such topological constraint, we may add a topological mutual BF term in the action that is
From and . The induced topological mutual BF term is linear in the conventional strength in and . This term is becomes
Next, we use Lagrangian approach to characterize the deformation of a knot (an SO(3)/SO(2) topological defect) on 2 + 1D space-time, . Using the similar approach, we derive another topological mutual BF term in the action that is
where . From and , this term becomes
The upper index of denotes entanglement transformation along given direction in winding space-time. We unify the index order of space-time into and reorganize the upper index. The topological mutual BF term becomes . In Ref. [16, 17, 18, 19], a topological description of Einstein-Hilbert action is proposed by S. W. MacDowell and F. Mansouri. The topological mutual BF term proposed in this paper is quite different from the MacDowell-Mansouri action.
According to the diffeomorphism invariance of winding space-time, there exists symmetry between the entanglement transformation along different directions. Therefore, with the help of a complete set of definition of reduced Gamma matrices , there exist other topological mutual BF terms . For the total topological mutual BF term that characterizes the deformation of a knot (an SO(4)/SO(3) topological defect) on a 3 + 1D zero-lattice, the upper index of the topological mutual BF term must be symmetric, i.e., .
By considering the SO(3,1) Lorentz invariance, the topological mutual BF term turns into the Einstein-Hilbert action as
where is the induced Newton constant which is . The role of the Planck length is played by , that is the “lattice” constant on the 3 + 1D zero-lattice.
Finally, from above discussion, we derived an effective theory of knots on deformed zero-lattice in continuum limit as
where . The variation of the action via the metric gives the Einstein’s equations
As a result, in continuum limit a knot-crystal becomes a space-time background like smooth manifold with emergent Lorentz invariance, of which the effective gravity theory turns into
For emergent gravity in knot physics, an important property is topological interplay between zero-lattice and knots. From the Einstein-Hilbert action, we found that the key property is duality between Riemann curvature and strength of auxiliary gauge field :
In addition, there exist a natural energy cutoff and a natural length cutoff . In high energy limit () or in short range limit (), without well-defined 3 + 1D zero-lattice, there does not exist emergent gravity at all.
6. Discussion and conclusion
In this paper, we pointed out that owing to the existence of local Lorentz invariance and diffeomorphism invariance there exists emergent gravity for knots on 3 + 1D zero-lattice. In knot physics, the emergent gravity theory is really a topological theory of entanglement deformation. For emergent gravity theory in knot physics, a topological interplay between 3 + 1D zero-lattice and the knots appears: on the one hand, the deformation of the 3 + 1D zero-lattice leads to the changes of knot-motions that can be denoted by curved space-time; on the other hand, the knots trapping topological defects deform the 3 + 1D zero-lattice that indicates matter may curve space-time. The Einstein-Hilbert action becomes a topological mutual BF term that exactly reproduces the low energy physics of the general relativity. In Table 1 , we emphasize the relationship between modern physics and knot physics.
|Modern physics||Knot physics|
|Matter||Knot: a topological defect of 3 + 1 D zero-lattice|
|Motion||Changing of the distribution of knot-pieces|
|Mass||Angular frequency for leapfrogging motion|
|Inertial reference system||A knot under Lorentz boosting|
|Coordinate translation||Entanglement transformation|
|Space-time||3 + 1D zero-lattice of projected entangled vortex-membranes|
|Curved space-time||Deformed 3 + 1D zero-lattice|
|Gravity||Topological interplay between 3 + 1D zero-lattice and knots|
In addition, this work would help researchers to understand the mystery in gravity. In modern physics, matter and space-time are two
One can see that matter (knots) and space-time (zero-lattice) together with motion of matter are
In the end of the paper, we address the possible physical realization of a 1D knot-crystal based on quantized vortex-lines in 4He superfluid. Because the emergent gravity in knot physics is topological interplay between zero-lattice and knots, there is no Einstein gravity on a 1D knot-crystal based on entangled vortex-lines in 4He superfluid. However, the curved space-time could be simulated.
Firstly, we consider two straight vortex-lines in 4He superfluid between opposite points on the system. Then, we rotate one vortex line around another by a rotating velocity . Now, the winding vortex-line becomes a helical one described by with . As a result, a knot-crystal is realized. For 4He superfluid, is the discreteness of the circulation owing to its quantum nature . is Planck constant and is atom mass of SF. So is about cm2/s. The length of the half pitch of the windings is set to be cm, and the distance between two vortex lines is set to be cm. We then estimate the effective light speed that is defined by (denotes the vortex filament radius which is much smaller than any other characteristic size in the system). The effective light speed is about 4 m/s. A non-uniform winding length leads to an effective curved 1 + 1D space-time.
However, at finite temperature, there exist mutual friction and phonon radiation for Kelvin waves on quantized vortex-lines in 4He superfluid. After considering these dissipation effects, the Kelvin waves are subject to Kolmogorov-like turbulence (even in quantum fluid [3, 4]).
This work is supported by NSFC Grant No. 11674026.