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 |
|---|---|---|---|---|---|---|---|---|---|
| 4253 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{2}M_{8}$ | 0.6354 | 0.7898 | 0.8045 | [M:[1.1765, 0.7451, 0.8235, 0.8235, 1.1765, 0.7843, 0.7059, 1.2549], q:[0.8039, 0.451], qb:[0.3725, 0.8039], phi:[0.3922]] | [M:[[-6], [-14], [6], [6], [-6], [-4], [-24], [14]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 | {a: 1469/2312, c: 913/1156, M1: 20/17, M2: 38/51, M3: 14/17, M4: 14/17, M5: 20/17, M6: 40/51, M7: 12/17, M8: 64/51, q1: 41/51, q2: 23/51, qb1: 19/51, qb2: 41/51, phi1: 20/51} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{8}$, ${ }q_{1}q_{2}$, ${ }M_{7}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{7}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}q_{1}q_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ | ${}M_{3}M_{5}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | -1 | t^2.118 + 2*t^2.353 + t^2.471 + t^3.412 + 2*t^3.529 + 2*t^3.765 + t^4.235 + 2*t^4.471 + t^4.588 + 3*t^4.706 + 3*t^4.824 + t^4.941 + t^5.529 + 2*t^5.647 + t^5.765 + 5*t^5.882 - t^6. + 2*t^6.118 + t^6.235 + t^6.353 + 2*t^6.588 + t^6.706 + 4*t^6.824 + 4*t^6.941 + 5*t^7.059 + 3*t^7.176 + 2*t^7.294 - 2*t^7.412 + 2*t^7.529 + t^7.647 + 2*t^7.765 + t^7.882 + 5*t^8. + 5*t^8.235 - t^8.353 + 2*t^8.706 + t^8.824 + 4*t^8.941 - t^4.176/y - t^6.294/y - (2*t^6.529)/y + (2*t^7.471)/y + t^7.588/y + t^7.706/y + (4*t^7.824)/y + t^8.059/y - t^8.412/y + t^8.529/y + (2*t^8.765)/y + (4*t^8.882)/y - t^4.176*y - t^6.294*y - 2*t^6.529*y + 2*t^7.471*y + t^7.588*y + t^7.706*y + 4*t^7.824*y + t^8.059*y - t^8.412*y + t^8.529*y + 2*t^8.765*y + 4*t^8.882*y | t^2.118/g1^24 + (2*t^2.353)/g1^4 + g1^6*t^2.471 + t^3.412/g1^16 + (2*t^3.529)/g1^6 + 2*g1^14*t^3.765 + t^4.235/g1^48 + (2*t^4.471)/g1^28 + t^4.588/g1^18 + (3*t^4.706)/g1^8 + 3*g1^2*t^4.824 + g1^12*t^4.941 + t^5.529/g1^40 + (2*t^5.647)/g1^30 + t^5.765/g1^20 + (5*t^5.882)/g1^10 - t^6. + 2*g1^10*t^6.118 + g1^20*t^6.235 + t^6.353/g1^72 + (2*t^6.588)/g1^52 + t^6.706/g1^42 + (4*t^6.824)/g1^32 + (4*t^6.941)/g1^22 + (5*t^7.059)/g1^12 + (3*t^7.176)/g1^2 + 2*g1^8*t^7.294 - 2*g1^18*t^7.412 + 2*g1^28*t^7.529 + t^7.647/g1^64 + (2*t^7.765)/g1^54 + t^7.882/g1^44 + (5*t^8.)/g1^34 + (5*t^8.235)/g1^14 - t^8.353/g1^4 + t^8.471/g1^96 - g1^6*t^8.471 + (2*t^8.706)/g1^76 + t^8.824/g1^66 + (4*t^8.941)/g1^56 - t^4.176/(g1^2*y) - t^6.294/(g1^26*y) - (2*t^6.529)/(g1^6*y) + (2*t^7.471)/(g1^28*y) + t^7.588/(g1^18*y) + t^7.706/(g1^8*y) + (4*g1^2*t^7.824)/y + (g1^22*t^8.059)/y - t^8.412/(g1^50*y) + t^8.529/(g1^40*y) + (2*t^8.765)/(g1^20*y) + (4*t^8.882)/(g1^10*y) - (t^4.176*y)/g1^2 - (t^6.294*y)/g1^26 - (2*t^6.529*y)/g1^6 + (2*t^7.471*y)/g1^28 + (t^7.588*y)/g1^18 + (t^7.706*y)/g1^8 + 4*g1^2*t^7.824*y + g1^22*t^8.059*y - (t^8.412*y)/g1^50 + (t^8.529*y)/g1^40 + (2*t^8.765*y)/g1^20 + (4*t^8.882*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2256 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{4}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ | 0.6548 | 0.8265 | 0.7923 | [M:[1.1725, 0.7357, 0.8275, 0.8275, 1.1725, 0.7816, 0.6898], q:[0.8046, 0.4597], qb:[0.3679, 0.8046], phi:[0.3908]] | t^2.069 + t^2.207 + 2*t^2.345 + t^2.483 + t^3.38 + 2*t^3.517 + t^3.793 + t^4.139 + t^4.277 + 3*t^4.414 + 3*t^4.552 + 4*t^4.69 + 3*t^4.828 + t^4.965 + t^5.449 + 3*t^5.587 + 3*t^5.725 + 4*t^5.862 - t^4.172/y - t^4.172*y | detail |