QKD: More text on mesh types
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1 changed files with 39 additions and 12 deletions
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@ -826,6 +826,11 @@ approximately \qty{11}{\milli\meter} when using minimal overlap between tab heig
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views.}
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\end{figure}
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In QKD applications, the simple disc cover design shown above has two main limitations. First, the distance between the
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primary and secondary meshes' tab rings must be large enough to allow for the fibers' minimum bend radius, resulting in
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more than \qty{10}{\milli\meter} of space available to an attacker. Second, the attacker only has to bend their tool in
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a plane to reach the payload.
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To increase the difficulty of inserting a long and flexible tool through the axis shield, \todo{Axis shield might be a
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nice term. Unify terminology for axis/shaft, the shield, the names of the two meshes, and the tabs sticking up from the
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meshes. Also what do we call the space in between? Terminology for the sides with offset meshes?} the shape of the
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@ -875,13 +880,23 @@ achieve or even exceed this standard with our work in the following sections.
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\label{qkd_fig_vault_door}
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\end{figure}
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Designing this type of labyrinth mesh is similar to the design of the shape of the jamb of a safe door such as the one
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shown in Figure\ \ref{qkd_fig_vault_door}, or of a high end apartment door. In these, the objective is to prevent
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would-be burglars from inserting opening tools through the space between the closed door and its jamb and attacking the
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door's interior handle or locking mechanism, not unlike an IHSM's defense against electrical or electromagnetic probes.
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The one difference between these doors and what we can do in IHSMs is that these doors are limited to outwards-facing
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steps because they must be opened and closed. In IHSM labyrinth meshes, we can use both outwards-facing and
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inwards-facing steps.
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While long and narrow tabs are desirable for mesh security as they limit the size and mobility of an attacker's probe,
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in QKD application, the need for fiber optic passthrough is the limiting factor. The obvious solution of passing through
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the fibers in a series of in-plane S-bends requires a coarse tab spacing due to the fibers' large minimum bend radius.
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However, we can apply the approach we proposed above for the shaft entrance here, too, and thread the fibers between the
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meshes by helically coiling them, increasing the fibers' bend radius to one half of the distance between both mesh
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discs minus the fibers' diameter and clearances\todo{Formulas here and elsewhere, define variables}. When the resulting
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useable part of the distance is larger than twice the bend radius, the minimum tab spacing is only limited by the
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fiber's diameter and the stability of the star bracket. When the discs are placed closer, and a larger pitch is
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necssary, the resulting pitch of the helix determines the minimum tab spacing.
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Designing a labyrinth mesh for intrusion prevention is similar to the design of the shape of the jamb of a safe door
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such as the one shown in Figure\ \ref{qkd_fig_vault_door}, or of a high end apartment door. In these, the objective is
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to prevent would-be burglars from inserting opening tools through the space between the closed door and its jamb and
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attacking the door's interior handle or locking mechanism, not unlike an IHSM's defense against electrical or
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electromagnetic probes. The one difference between these doors and what we can do in IHSMs is that these doors are
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limited to outwards-facing steps because they must be opened and closed. In IHSM labyrinth meshes, we can use both
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outwards-facing and inwards-facing steps.
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Concentric labyrinth meshes allow for a wide range of different configurations. The pitch from one mesh tab to the
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next is the sum of the required width of the inter-mesh space and the safety margin needed betwween any cables or the
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@ -930,11 +945,23 @@ and axial dimensions as illustrated in Figure\ \ref{qkd_fig_mesh_ring_bearing_to
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\label{qkd_fig_offset_lab_schema}
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\end{figure}
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In QKD applications, the simple disc cover design shown above has two main limitations. First, the distance between the
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primary and secondary meshes' tab rings must be large enough to allow for the fibers' minimum bend radius, resulting in
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more than \qty{10}{\milli\meter} of space available to an attacker. Second, the attacker only has to bend their tool in
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a plane to reach the payload. In this section, we will show a design and a mechanical prototype of an offset labyrinth
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mesh design that improves both of these quantities.
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Concentric labyrinth meshes improve upon simple disc meshes in security, but they have two remaining weaknesses. One is
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that in a concentric labyrinth mesh, the part of the inner mesh at the axis is easily accessible through the opening in
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the outer mesh. As the axis of rotation is the most vulnerable spot in a mesh because the tangential velocity of the
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mesh is lowest close to the axis, tampering can be made more difficult by placing the axis of rotation of the inner mesh
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not concentric with that of the outer mesh, but at a radial \emph{offset}.
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A consequence of placing the axis of the inner mesh at an offset is that the inter-mesh rings formed by the tabs of the
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two meshes now no longer form a set of concentric rings, but a set of nested non-concentric annulus shapes whose narrow
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and wide sides alternate along the direction of the offset. We will show below how an optical fiber can still be wound
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through this complex inter-mesh space without much trouble through a variation of the helical spiral trick from above to
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avoid the annular rings' narrow sections. At the same time, the alternating narrow sections of the annular rings make it
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more difficult to feed through the type of surgical robot we cited above, whose joints are designed for in-plane
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operation for most of the manipulator, starting from the high-flexibility joints close to its end and down the neck. In
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this section, we will show a design and a mechanical prototype of an offset labyrinth mesh design that improves on a
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concentric labyrinth mesh on both the shielding of the secondary mesh axis and the feasibility of an attack with a
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surgical robot without increasing mechanical complexity compared to a concentric design. In addition, we show a fiber
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feedthrough that improves on the simple helical feedthrough we introduced above.
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\begin{figure}
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\centering
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