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 |
|---|---|---|---|---|---|---|---|---|---|
| 4618 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{8}q_{1}\tilde{q}_{2}$ | 0.709 | 0.8809 | 0.8049 | [M:[1.0833, 0.75, 0.875, 0.9583, 1.0417, 0.7917, 1.25, 0.7917], q:[0.5417, 0.375], qb:[0.5833, 0.6667], phi:[0.4583]] | [M:[[-2], [6], [15], [-11], [11], [-7], [-6], [-7]], q:[[-1], [3]], qb:[[-14], [8]], phi:[[1]]] | 1 | {a: 363/512, c: 451/512, M1: 13/12, M2: 3/4, M3: 7/8, M4: 23/24, M5: 25/24, M6: 19/24, M7: 5/4, M8: 19/24, q1: 13/24, q2: 3/8, qb1: 7/12, qb2: 2/3, phi1: 11/24} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{8}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{8}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{6}$, ${ }M_{5}M_{8}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{3}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -2 | 2*t^2.375 + t^2.625 + t^2.75 + t^2.875 + t^3.125 + t^3.25 + t^3.75 + t^4.125 + t^4.25 + t^4.5 + t^4.625 + 4*t^4.75 + t^4.875 + 3*t^5. + 2*t^5.125 + 3*t^5.25 + t^5.375 + 3*t^5.5 + 2*t^5.625 + t^5.75 + t^5.875 - 2*t^6. + 2*t^6.125 + t^6.375 + t^6.5 + 2*t^6.625 + 2*t^6.875 + 3*t^7. + 7*t^7.125 + 3*t^7.25 + 5*t^7.375 + 5*t^7.5 + 7*t^7.625 + 3*t^7.75 + 5*t^7.875 + 5*t^8. + 3*t^8.125 + 2*t^8.25 - 4*t^8.375 + 5*t^8.5 - 2*t^8.625 - t^8.875 - t^4.375/y - (2*t^6.75)/y - t^7./y + (2*t^7.75)/y + (4*t^8.)/y + (2*t^8.125)/y + (2*t^8.25)/y + t^8.375/y + (3*t^8.5)/y + (3*t^8.625)/y + t^8.75/y + (2*t^8.875)/y - t^4.375*y - 2*t^6.75*y - t^7.*y + 2*t^7.75*y + 4*t^8.*y + 2*t^8.125*y + 2*t^8.25*y + t^8.375*y + 3*t^8.5*y + 3*t^8.625*y + t^8.75*y + 2*t^8.875*y | (2*t^2.375)/g1^7 + g1^15*t^2.625 + g1^2*t^2.75 + t^2.875/g1^11 + g1^11*t^3.125 + t^3.25/g1^2 + t^3.75/g1^6 + g1^3*t^4.125 + t^4.25/g1^10 + g1^12*t^4.5 + t^4.625/g1 + (4*t^4.75)/g1^14 + t^4.875/g1^27 + 3*g1^8*t^5. + (2*t^5.125)/g1^5 + (2*t^5.25)/g1^18 + g1^30*t^5.25 + g1^17*t^5.375 + 3*g1^4*t^5.5 + (2*t^5.625)/g1^9 + g1^26*t^5.75 + g1^13*t^5.875 - 2*t^6. + (2*t^6.125)/g1^13 + g1^9*t^6.375 + t^6.5/g1^4 + (2*t^6.625)/g1^17 + 2*g1^5*t^6.875 + (3*t^7.)/g1^8 + (6*t^7.125)/g1^21 + g1^27*t^7.125 + (2*t^7.25)/g1^34 + g1^14*t^7.25 + 5*g1*t^7.375 + (5*t^7.5)/g1^12 + (4*t^7.625)/g1^25 + 3*g1^23*t^7.625 + t^7.75/g1^38 + 2*g1^10*t^7.75 + (4*t^7.875)/g1^3 + g1^45*t^7.875 + (4*t^8.)/g1^16 + g1^32*t^8. + 3*g1^19*t^8.125 + 2*g1^6*t^8.25 - (5*t^8.375)/g1^7 + g1^41*t^8.375 + (3*t^8.5)/g1^20 + 2*g1^28*t^8.5 + t^8.625/g1^33 - 3*g1^15*t^8.625 - t^8.875/g1^11 - (g1*t^4.375)/y - (2*t^6.75)/(g1^6*y) - (g1^16*t^7.)/y + (2*t^7.75)/(g1^14*y) + (4*g1^8*t^8.)/y + (2*t^8.125)/(g1^5*y) + (2*t^8.25)/(g1^18*y) + (g1^17*t^8.375)/y + (3*g1^4*t^8.5)/y + (3*t^8.625)/(g1^9*y) + (g1^26*t^8.75)/y + (2*g1^13*t^8.875)/y - g1*t^4.375*y - (2*t^6.75*y)/g1^6 - g1^16*t^7.*y + (2*t^7.75*y)/g1^14 + 4*g1^8*t^8.*y + (2*t^8.125*y)/g1^5 + (2*t^8.25*y)/g1^18 + g1^17*t^8.375*y + 3*g1^4*t^8.5*y + (3*t^8.625*y)/g1^9 + g1^26*t^8.75*y + 2*g1^13*t^8.875*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2553 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ | 0.6922 | 0.8511 | 0.8133 | [M:[1.0852, 0.7445, 0.8612, 0.9685, 1.0315, 0.7981, 1.2555], q:[0.5426, 0.3722], qb:[0.5962, 0.6593], phi:[0.4574]] | t^2.394 + t^2.584 + t^2.744 + t^2.905 + t^3.095 + t^3.256 + t^3.606 + t^3.767 + t^4.117 + t^4.278 + t^4.467 + t^4.628 + 2*t^4.789 + t^4.95 + 2*t^4.978 + t^5.139 + t^5.167 + t^5.3 + t^5.328 + 2*t^5.489 + t^5.65 + t^5.678 + t^5.839 - t^6. - t^4.372/y - t^4.372*y | detail |