Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 4908 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{5}M_{8}$ + ${ }M_{6}^{2}$ | 0.6958 | 0.8525 | 0.8162 | [M:[0.9698, 1.0, 1.0151, 0.9546, 1.0454, 1.0, 1.0151, 0.9546], q:[0.5302, 0.5], qb:[0.4546, 0.5454], phi:[0.4924]] | [M:[[-4], [0], [2], [-6], [6], [0], [2], [-6]], q:[[4], [0]], qb:[[-6], [6]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{8}$, ${ }M_{1}$, ${ }M_{6}$, ${ }M_{3}$, ${ }M_{7}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{8}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{3}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{7}$ | ${}$ | -3 | 2*t^2.864 + t^2.909 + t^3. + 2*t^3.045 + t^3.227 + t^4.205 + t^4.341 + t^4.432 + 2*t^4.477 + t^4.568 + t^4.613 + t^4.659 + t^4.704 + t^4.749 + 2*t^5.728 + t^5.773 + t^5.819 + 4*t^5.909 + t^5.955 - 3*t^6. + t^6.045 + 3*t^6.091 - t^6.136 + t^6.272 + t^6.454 + 2*t^7.069 + t^7.114 + 2*t^7.205 + t^7.251 + t^7.296 + 3*t^7.341 + 2*t^7.387 + t^7.432 + 2*t^7.477 + 3*t^7.523 + t^7.568 + 2*t^7.613 + 3*t^7.659 + t^7.704 + t^7.749 + t^7.795 + t^7.886 + t^7.931 + t^7.976 + t^8.41 + t^8.546 + 2*t^8.592 + t^8.637 + 3*t^8.682 + 3*t^8.773 + 4*t^8.819 - 4*t^8.864 - 2*t^8.909 + 6*t^8.955 - t^4.477/y - t^7.341/y - t^7.387/y + t^7.432/y - t^7.523/y + t^7.568/y + t^7.613/y + t^8.728/y + (2*t^8.773)/y + (2*t^8.864)/y + (5*t^8.909)/y + (2*t^8.955)/y - t^4.477*y - t^7.341*y - t^7.387*y + t^7.432*y - t^7.523*y + t^7.568*y + t^7.613*y + t^8.728*y + 2*t^8.773*y + 2*t^8.864*y + 5*t^8.909*y + 2*t^8.955*y | (2*t^2.864)/g1^6 + t^2.909/g1^4 + t^3. + 2*g1^2*t^3.045 + g1^10*t^3.227 + t^4.205/g1^13 + t^4.341/g1^7 + t^4.432/g1^3 + (2*t^4.477)/g1 + g1^3*t^4.568 + g1^5*t^4.613 + g1^7*t^4.659 + g1^9*t^4.704 + g1^11*t^4.749 + (2*t^5.728)/g1^12 + t^5.773/g1^10 + t^5.819/g1^8 + (4*t^5.909)/g1^4 + t^5.955/g1^2 - 3*t^6. + g1^2*t^6.045 + 3*g1^4*t^6.091 - g1^6*t^6.136 + g1^12*t^6.272 + g1^20*t^6.454 + (2*t^7.069)/g1^19 + t^7.114/g1^17 + (2*t^7.205)/g1^13 + t^7.251/g1^11 + t^7.296/g1^9 + (3*t^7.341)/g1^7 + (2*t^7.387)/g1^5 + t^7.432/g1^3 + (2*t^7.477)/g1 + 3*g1*t^7.523 + g1^3*t^7.568 + 2*g1^5*t^7.613 + 3*g1^7*t^7.659 + g1^9*t^7.704 + g1^11*t^7.749 + g1^13*t^7.795 + g1^17*t^7.886 + g1^19*t^7.931 + g1^21*t^7.976 + t^8.41/g1^26 + t^8.546/g1^20 + (2*t^8.592)/g1^18 + t^8.637/g1^16 + (3*t^8.682)/g1^14 + (3*t^8.773)/g1^10 + (4*t^8.819)/g1^8 - (4*t^8.864)/g1^6 - (2*t^8.909)/g1^4 + (6*t^8.955)/g1^2 - t^4.477/(g1*y) - t^7.341/(g1^7*y) - t^7.387/(g1^5*y) + t^7.432/(g1^3*y) - (g1*t^7.523)/y + (g1^3*t^7.568)/y + (g1^5*t^7.613)/y + t^8.728/(g1^12*y) + (2*t^8.773)/(g1^10*y) + (2*t^8.864)/(g1^6*y) + (5*t^8.909)/(g1^4*y) + (2*t^8.955)/(g1^2*y) - (t^4.477*y)/g1 - (t^7.341*y)/g1^7 - (t^7.387*y)/g1^5 + (t^7.432*y)/g1^3 - g1*t^7.523*y + g1^3*t^7.568*y + g1^5*t^7.613*y + (t^8.728*y)/g1^12 + (2*t^8.773*y)/g1^10 + (2*t^8.864*y)/g1^6 + (5*t^8.909*y)/g1^4 + (2*t^8.955*y)/g1^2 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 2701 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{5}M_{8}$ | 0.6971 | 0.8562 | 0.8141 | [M:[0.9343, 1.0398, 1.0129, 0.9613, 1.0387, 0.9602, 1.0129, 0.9613], q:[0.5457, 0.5199], qb:[0.4413, 0.5188], phi:[0.4935]] | t^2.803 + t^2.881 + 2*t^2.884 + 2*t^3.039 + t^3.194 + t^4.129 + t^4.361 + t^4.364 + t^4.442 + t^4.594 + t^4.597 + t^4.6 + t^4.674 + t^4.678 + t^4.755 + t^5.606 + t^5.684 + t^5.687 + t^5.761 + t^5.764 + 2*t^5.768 + 2*t^5.842 + t^5.919 + 3*t^5.923 - 4*t^6. - t^4.481/y - t^4.481*y | detail |